Obtaining information from optical cavity output light

ABSTRACT

Output light from an optical cavity includes, for each of a set of modes, an intensity function, and a mode&#39;s intensity function includes information, such as about an optical characteristic of an analyte or of a region. For example, the intensity function can include a peak, and its central energy, maximum intensity, contrast, or intermediate intensity width (e.g. FWHM) can indicate the optical characteristic. The output light can be photosensed, providing electrical signals that depend on the optical characteristic. Information about the analyte or region can then be obtained using the electrical signals. For example, the information can be about both refractive index and absorption of an analyte. Cavity-only absorption values, independent, for example, of absorption outside the cavity and of inhomogeneous illumination, can be obtained based on contrast or intermediate intensity width. For detection of glucose in bodily fluid, derivatives of absorption can be obtained.

This application is related to the following applications, each of which is hereby incorporated by reference in its entirety: “Chip-Size Wavelength Detector”, U.S. patent application Ser. No. 10/922,870, now published as U.S. Patent Application Publication No. 2006/0039009; “Sensing Photon Energies Emanating From Channels or Moving Objects”, U.S. patent application Ser. No. 11/315,992; “Photosensing Throughout Energy Range and in Subranges”, U.S. patent application Ser. No. 11/316,438; “Obtaining Analyte Information”, U.S. patent application Ser. No. 11/316,303; “Position-Based Response to Light”, U.S. patent application Ser. No. 11/633,302; “Photosensing Optical Cavity Output Light”, U.S. patent application Ser. No. 11/702,250; “Encoding Optical Cavity Output Light”, U.S. patent application Ser. No. 11/702,363; “Distinguishing Objects”, U.S. patent application Ser. No. 11/702,328; “Moving Analytes and Photosensors”, U.S. patent application Ser. No. 11/702,470; and “Implanting Optical Cavity Structures”, U.S. patent application Ser. No. 11/702,329; “Containing Analyte In Optical Cavity Structures”, U.S. patent application Ser. No. 11/702,325; “Tuning Optical Cavities”, U.S. patent application Ser. No. 11/702,321; and “Tuning Optical Cavities”, U.S. patent application Ser. No. 11/702,320.

BACKGROUND OF THE INVENTION

The present invention relates generally to techniques involving optical cavities, such as techniques that obtain information from output light from optical cavities.

Liang X. J., Liu, A. Q., Zhang, X. M., Yap, P. H., Ayi, T. C., and Yoon, H. S., “Refractive Index Measurement of Single Living Cell Using a Biophotonic Chip for Cancer Diagnosis Applications,” 9^(th) International Conference on Miniaturized Systems for Chemistry and Life Sciences, Oct. 9-13, 2005, Boston, Mass., 2005, pp. 464-466 describe techniques that perform refractive index (RI) measurement of single living cells using a biophotonic chip for cancer diagnosis applications. Liang et al. describe a biophotonic chip that is formed by bonding a metal-coated glass slide with a PDMS slab molded using soft lithography technology. An analysis unit embedded in the chip to measure RI includes a laser diode with one surface opposite a gold-coated mirror, forming an external laser cavity. A microlens array in the chip improves beam quality, and living cells in a buffer are driven by electrokinetic force and delivered into an analysis region along microfluidic channels. A difference in RI between a cell and the buffer changes the effective cavity length so that laser emission varies, with a wavelength shift. The cell's effective RI can be computed by monitoring wavelength and power.

Table 1 from Liang shows a number of exemplary refractive indices relevant to cancerous cells.

TABLE 1 Cell Type Refractive Index Culture medium 1.350 HeLa 1.392 PC12 1.395 MDA-MB-231 1.399 MCF-7 1.401 Jurkat 1.390

Liang et al. state that automatic measurement of RI of a living cell in real time offers low cost, high accuracy disease diagnosis.

It would be advantageous to have improved techniques for optical cavities, including improved techniques for obtaining information from optical cavity output light.

SUMMARY OF THE INVENTION

The invention provides various exemplary embodiments, including systems, methods, apparatus, and devices. In general, the embodiments involve obtaining information from one or more modes of optical cavity output light.

These and other features and advantages of exemplary embodiments of the invention are described below with reference to the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic diagram of a system in which information is obtained from modes of output light from an optical cavity.

FIG. 2 is a schematic side view of a homogeneous optical cavity that could be used in the system of FIG. 1.

FIG. 3 is a graph showing intensity-energy curves for transmission and reflection from a cavity as in FIG. 2 when operated as a Fabry-Perot cavity, showing ways in which information can be included in transmission mode peaks.

FIG. 4 is a schematic side view of a graded optical cavity that is an example of an inhomogeneous optical cavity that could be used in the system of FIG. 1.

FIG. 5 is a graph showing an intensity-position function of a cavity as in FIG. 4, showing both spectral and harmonic relationships between peaks.

FIG. 6 is a schematic diagram of a setup in which an optical cavity as in FIG. 2 or 4 could operate to provide output light with reflection modes.

FIG. 7 is a schematic diagram of an implementation of the system of FIG. 1.

FIG. 8 is a schematic circuit diagram of a system implemented as in FIG. 7.

FIG. 9 is a flow diagram showing operations of the analyte information routine in FIG. 8.

FIG. 10 is a schematic top view of a device that can be used in a system implemented as in FIGS. 7 and 8.

FIG. 11 is a schematic cross section of the device of FIG. 10, taken along the line 11-11.

FIG. 12 is a graph showing two transmission spectra that could be obtained from a device as in FIGS. 10 and 11 with analytes having different refractive indices.

FIG. 13 includes two graphs showing two transmission spectra that could be obtained from a device as in FIGS. 10 and 11 with an analyte absent and present, with the second graph providing an absorption spectrum for the analyte.

FIG. 14 is a schematic top view of a multiple channel device that can be used in a system implemented as in FIGS. 7 and 8.

FIG. 15 is a schematic cross section of the device of FIG. 14, taken along the line 15-15.

FIG. 16 is a flowchart showing operations in producing devices as in FIGS. 10, 11, 14, and 15.

FIG. 17 is a schematic top view of components of an implementation of a system as in FIGS. 7 and 8 in which relative motion occurs between a biochip with an array of analyte-containing wells or locations and a photosensing array.

FIG. 18 is a schematic diagram of a setup that could be used in an implementation of a system as in FIGS. 7 and 8 in which analyte-containing objects such as biological cells pass through a laser cavity.

FIG. 19 is a schematic side view of a graded optical cavity that can contain analyte and could be used in a system as in FIGS. 7 and 8.

FIG. 20 is a schematic top view of a photosensing component as in FIG. 19.

FIG. 21 is a schematic side view of an optical cavity that can be tuned by modifying the length of elastomer spacers and could be used in a system as in FIGS. 7 and 8.

FIG. 22 is a graph showing two transmission spectra that could be provided by tuning an optical cavity as in FIG. 21.

FIG. 23 is a schematic diagram of an analyzer on a fluidic structure, where the analyzer includes a system implemented as in FIGS. 7 and 8.

FIG. 24 is a schematic diagram of an implementation of a system as in FIGS. 7 and 8 that can monitor analyte in bodily fluid.

FIG. 25 is a graph showing normalized intensity as a function of photon energy for a transmission spectrum of an optical cavity with a given refractive index and for sensing spectra of several cells of a photosensing array as in the system of FIGS. 7 and 8 or another system.

FIG. 26 is a graph showing normalized intensity as a function of photon energy for a transmission spectrum of the same optical cavity as in FIG. 25 but with a different given refractive index and for the same sensing spectra as in FIG. 25.

FIG. 27 is a graph showing transmitted intensity as a function of photon energy with different amounts of absorption as in an optical cavity like that of FIG. 13.

FIG. 28 is a graph showing transmitted intensity as a function of photon energy with different amounts of absorption as in FIG. 27, but with transmitted intensity normalized.

FIG. 29 is a graph showing plotted values of relative change in transmittance as a function of absorption for several reflectivities in an optical cavity filled with air.

FIG. 30 is a graph showing plotted values of an enhancement factor as a function of absorption for several reflectivities in the same optical cavity as FIG. 29, again filled with air.

FIG. 31 is a graph showing plotted values of relative change in transmittance as a function of absorption for several reflectivities in the same optical cavity as FIGS. 29 and 30 but filled with water.

FIG. 32 is a graph showing plotted values of an enhancement factor as in FIG. 30, obtained as a function of absorption for several reflectivities in the same optical cavity as FIGS. 29-31, again filled with water.

FIG. 33 is a graph showing intensity as a function of photosensing cell position for three peaks with the same central energy but different FWHMs.

DETAILED DESCRIPTION

In the following detailed description, numeric values and ranges are provided for various aspects of the implementations described. These values and ranges are to be treated as examples only, and are not intended to limit the scope of the claims. In addition, a number of materials are identified as suitable for various facets of the implementations. These materials are to be treated as exemplary, and are not intended to limit the scope of the claims.

“Light” refers herein to electromagnetic radiation of any wavelength or frequency; unless otherwise indicated, a specific value for light wavelength or frequency is that of light propagating through vacuum. The term “photon” refers herein to a quantum of light, and the term “photon energy” refers herein to the energy of a photon. Light can be described as having a “photon energy distribution”, meaning the combination of photon energies that are included in the light; highly monochromatic light, for example, has a photon energy distribution with one peak energy value. A photon energy distribution can be specified in space and time: For example, a photon energy distribution can be specified as a function of position, such as on a surface, or as a function of time; a photon energy distribution that is “homogeneous” is substantially the same at all relevant positions, such as the positions of a surface, while a photon energy distribution that is “stable” is substantially the same at all relevant times.

Light can also be described as provided by a “light source,” which, unless otherwise specified, refers herein to any device, component, or structure that can provide light of the type described; examples of light sources relevant to the below-described implementations include various kinds of pulsed and unpulsed lasers and laser structures, light emitting diodes (LEDs), superluminescent LEDs (SLEDs), resonant cavity LEDs, sources of broadband light that is spectrally filtered such as with a monochromator, and so forth. A “tunable light source” is a light source that provides light with a predominant photon energy that can be changed in response to a signal or operation of some kind.

The term “laser” is used herein to mean any region, element, component, or device in which transitions between energy levels can be stimulated to cause emission of coherent light, such as in the ultraviolet, visible, or infrared regions of the spectrum. A “laser structure” is any structure that includes one or more lasers. A “laser cavity” is a region of a laser in which transitions can be stimulated to cause emission.

To “propagate” light through a region or structure is to transmit or otherwise cause the light to propagate through the region or structure. The light may be referred to as “propagated light” or “propagating light”.

Propagating light can often be usefully characterized by direction and speed of propagation, with direction typically illustrated by one or more rays and with speed typically being described relative to the constant c, also referred to as the speed of light in vacuum. Where light changes direction in a way that can be illustrated as a vertex between an incoming ray and an outgoing ray, the change may be referred to as a “reflection”; similarly, to “reflect” light is to cause the light to change its direction of propagation approximately at a surface, referred to herein as a “reflection surface”. Where light propagates at less than c, it may be useful to obtain an “optical distance” of propagation; for any segment of length d in which speed of propagation is constant ε*c, where ε≦1, optical distance D(ε)=d/ε. An optical distance may be referred to herein as an “optical thickness”, such as where light is propagating through a thickness of material.

“Photon energy information” refers herein to information about photon energy, such as information about wavelength, frequency, wavelength shift, frequency shift, or a distribution of wavelengths or frequencies. “Absolute photon energy information” is information about a given photon energy value, such as a specific wavelength or frequency, while “relative photon energy information” is information that relates two photon energy values, whether measured concurrently or at different times.

To “photosense” is to sense photons, and to “photosense quantity” of photons is to obtain information indicating a quantity of the photons. Photons that are photosensed are sometimes referred to herein as “incident photons”. A surface at which photosensing occurs is referred to herein as a “photosensitive surface”.

A “photosensor” is used herein to refer generally to any element or combination of elements that senses photons, whether by photosensing quantity or any other information about the photons. A photosensor could, for example, provide an electrical signal or other signal that indicates results of sensing, such as a signal indicating quantity of incident photons; in general, signals from a photosensor that indicate results of sensing are referred to herein as “sensing results”. If electrical sensing events occur in a photosensor in response to incident photons, the photosensor may integrate or otherwise accumulate the results of the electrical sensing events during a time period referred to herein as a “sensing period” or “sense period”.

A “range of photon energies” or an “energy range” is a range of energy values that photons can have. An energy range can be described, for example, as a range of wavelengths or a range of frequencies or, in appropriate cases, by the range's central wavelength or frequency and possibly also the range's width. A “subrange” of a range of photon energies is a part of the range, and can be similarly described. A central wavelength or frequency or other value indicating a central photon energy of a range or subrange is sometimes referred to herein as a “central energy”, and may be obtained in various ways, such as by finding an energy that has maximum intensity or that is another type of central value such as a mean or median of the distribution of light within the range or subrange.

In general, the upper and lower boundaries and widths of ranges and subranges are approximate. To provide output photons or to photosense quantity of photons “throughout”, “within”, or “in” a range or subrange means to provide photons or to obtain information about quantity of photons that are predominantly within the range or subrange. In typical cases, between 60-90% of the provided photons or sensed quantity of photons have energies within the range or subrange, but the percentage could be lower or higher. In some applications, 90% or even 95% or more of the provided photons or sensed quantity of photons have energies within the range or subrange.

Some of the photosensing implementations described herein employ structures with one or more dimensions smaller than 1 mm, and various techniques have been proposed for producing such structures. In particular, some techniques for producing such structures are referred to as “microfabrication.” Examples of microfabrication include various techniques for depositing materials such as growth of epitaxial material, sputter deposition, evaporation techniques, plating techniques, spin coating, printing, and other such techniques; techniques for patterning materials, such as etching or otherwise removing exposed regions of thin films through a photolithographically patterned resist layer or other patterned layer; techniques for polishing, planarizing, or otherwise modifying exposed surfaces of materials; and so forth.

In general, the structures, elements, and components described herein are supported on a “support structure” or “support surface”, which terms are used herein to mean a structure or a structure's surface that can support other structures. More specifically, a support structure could be a “substrate”, used herein to mean a support structure on a surface of which other structures can be formed or attached by microfabrication or similar processes.

The surface of a substrate or other support surface is treated herein as providing a directional orientation as follows: A direction away from the surface is “up”, “over”, or “above”, while a direction toward the surface is “down”, “under”, or “below”. The terms “upper” and “top” are typically applied to structures, components, or surfaces disposed away from the surface, while “lower” or “underlying” are applied to structures, components, or surfaces disposed toward the surface. In general, it should be understood that the above directional orientation is arbitrary and only for ease of description, and that a support structure or substrate may have any appropriate orientation.

Unless the context indicates otherwise, the terms “circuitry” and “circuit” are used herein to refer to structures in which one or more electronic components have sufficient electrical connections to operate together or in a related manner. In some instances, an item of circuitry can include more than one circuit. An item of circuitry that includes a “processor” may sometimes be analyzed into “hardware” and “software” components; in this context, “software” refers to stored or transmitted data that controls operation of the processor or that is accessed by the processor while operating, and “hardware” refers to components that store, transmit, and operate on the data. The distinction between “software” and “hardware” is not always clear-cut, however, because some components share characteristics of both; also, a given software component can often be replaced by an equivalent hardware component without significantly changing operation of circuitry.

Circuitry can be described based on its operation or other characteristics. For example, circuitry that performs control operations is sometimes referred to herein as “control circuitry” and circuitry that performs processing operations is sometimes referred to herein as “processing circuitry”.

An “integrated circuit” or “IC” is a structure with electrical components and connections produced by microfabrication or similar processes. An IC may, for example, be on or over a substrate on which it was produced or another suitable support structure. Other components could be on the same support structure with an IC, such as discrete components produced by other types of processes.

Implementations of ICs described herein include features characterized as “cells” (or “elements”) and “arrays”, terms that are used with related meanings: An “array” is an arrangement of “cells” or “elements”; unless otherwise indicated by the context, such as for a biological cell, the words “cell” and “element” are used interchangeably herein to mean a cell or an element of an array. An array may also include circuitry that connects to electrical components within the cells such as to select cells or transfer signals to or from cells, and such circuitry is sometimes referred to herein as “array circuitry”. In contrast, the term “peripheral circuitry” is used herein to refer to circuitry on the same support surface as an array and connected to its array circuitry but outside the array. The term “external circuitry” is more general, including not only peripheral circuitry but also any other circuitry that is outside a given cell or array.

Some of the implementations below are described in terms of “rows” and “columns”, but these terms are interchangeable. Also, rows and columns are described herein as examples of “lines”. Within an array, a “line” of cells refers herein to a series of cells through which a line can be drawn without crossing areas of cells that are not in the line. For example, in a two-dimensional array in which cells have uniform areas, a line of cells could be a row, a column, a diagonal, or another type of straight line; more generally, a line of cells could be straight or could include one or more non-straight features, such as curves or angles.

An IC includes a “photosensor array” if the IC includes an array of cells, and at least some of the cells include respective photosensors. A cell that includes a photosensor may also include “cell circuitry”, such as circuitry that makes connections with the photosensor, that transfers signals to or from the photosensor, or that performs any other operation other than photosensing. In general, a cell's photosensor and cell circuitry are within a bounded area of the array, an area sometimes referred to herein as the “cell's area”. The part of a cell's area in which an incident photon can be photosensed is referred to herein as “sensing area”.

In an application of an IC that includes a photosensor array, circuitry that “responds to” one or more photosensors can be any circuitry that, in operation, receives information from the photosensors about their photosensing results through an electrical connection. Circuitry that responds to a photosensor could be circuitry in the same cell as the photosensor, or it could be array circuitry, peripheral circuitry, or other external circuitry, or it could include any suitable combination of cell circuitry, array circuitry, peripheral circuitry, and other external circuitry. Circuitry that responds to a photosensor could employ any suitable technique to read out photosensing results, including, for example, CCD, CMOS, or photodetector array (PDA) techniques.

An IC is or includes a “position-sensitive detector” or “PSD” if it includes a substantially continuous photosensitive surface and it provides electrical signals indicating a position resulting from a pattern of incident light on the photosensitive surface. For example, the signals could be two currents whose normalized difference is proportional to a centroid of the incident light pattern.

FIG. 1 illustrates general features of system 10, an example of a system that can be implemented as described in greater detail below. As with other implementations described below, system 10 involves a combination of parts or components. As used herein, a “system” is a combination of two or more parts or components that can perform an operation together. A system may be characterized by its operation: for example, an “analyte information system” is a system that operates somehow on analyte information; a “processing system” is a system that performs data or signal processing; and so forth.

Within a system, components and parts may be referred to in a similar manner. One component of an analyte information system in which information is obtained about an analyte's optical characteristics, for example, can be a “detector component” or simply “detector”, meaning a component that detects light; similarly, a “light source component” includes one or more light sources; an “optical component” performs an optical operation; a “photosensing component” performs a photosensing operation; an “information obtaining component” obtains information, such as from photosensing results; a “light-transmissive component” or simply “transmission component” transmits light; a “light-reflective component” or simply “reflective component” reflects light; and other examples are defined further below. Other parts or components can be characterized by their structure.

System 10 includes optical cavity component 12, photosensing component 14, and information obtaining component 16. Optical cavity component 12 includes optical cavity 20.

The term “reflective optical cavity”, or simply “optical cavity” or “cavity”, refers herein to a light-transmissive region that is at least partially bounded by light-reflective components, with the light-reflective components and the light-transmissive region having characteristics such that a measurable portion of light within the light-transmissive region is reflected more than once across the light-transmissive region. An “optical cavity component” is a component that includes one or more optical cavities.

Within the broad category of optical cavities, there are various more specific types: For example, a laser cavity, mentioned above, is an example of an “emitting optical cavity” or simply “emitting cavity” that can operate as a source of emitted output light even when it is not receiving input light from an external light source, with the emitted light ordinarily resulting from a gain medium within the light-transmissive region; similarly, a “transmissive cavity” can operate, in response to input light from one or more external light sources at an entry surface, providing a transmitted portion of its output light at an exit surface different than the entry surface (a complementary, reflected portion may be provided at the entry surface); a “Fabry-Perot cavity” is a reflective optical cavity in which constructive interference (or positive reinforcement) occurs in one or more photon energy subranges while destructive interference occurs in others.

The various exemplary implementations described below address problems that arise in obtaining information from output light of optical cavities. The implementations are especially relevant to output light that includes information about an optical characteristic, such as of an analyte or a region in the cavity's light-transmissive region. One problem is the difficulty of obtaining high resolution information about optical characteristics rapidly and without bulky, expensive equipment; absorption spectroscopy of analytes in fluid, for example, typically requires wavelength resolution 1-10 nm or better. This can not be achieved with simple filter-based optical systems; instead, bulky spectrometers are necessary. Another problem in absorption spectroscopy is that a long interaction length between light and analyte is required to detect small absorption changes, so that large sample chambers are necessary, which require a large amount of analyte. Another problem is that accurate information may be difficult to obtain because of various types of noise that may be present in an optical system. Yet another problem is that techniques used to obtain information for one optical characteristic are usually not adapted for another characteristic, so that several different techniques must be used to obtain information about several optical characteristics, e.g. to concurrently get information on refractive index and absorption properties.

A Fabry-Perot cavity or other optical cavity that can operate to provide output light in one or more photon energy subranges while not providing output light with other photon energies may be described as having one or more “modes”, each for a respective one of the output light energy subranges; if the cavity is a transmissive cavity, modes of its transmitted output light may be referred to as “transmission modes” and modes of its reflected output light may be referred to as “reflection modes”. In the reflection spectrum, either the valley-like dips or the plateau-like reflection bands between the dips can be considered as “reflection modes”. An emitting cavity can be described as “stimulated at” a mode by any operation that results in emission of output light in the mode's photon energy subrange. Similarly, a transmissive cavity can be described as “illuminated at” a mode by any operation that provides input light that results in transmission or reflection of output light in the mode's photon energy subrange.

In typical implementations of optical cavities; two light-reflective components have approximately parallel reflection surfaces and the light-transmissive region is sufficiently uniform that measurements would indicate many reflections of light within the light-transmissive region. Such cavities define a directional orientation as follows: Directions in which light could propagate and be reflected many times within the light-transmissive region are referred to herein as “reflection directions”, and generally include a range of directions that are approximately perpendicular to both reflection surfaces. Directions that are approximately parallel to both reflection surfaces, on the other hand, are generally referred to herein as “lateral directions”. In addition, the terms “in”, “inward”, or “internal” generally refer to positions, directions, and other items within or toward the light-transmissive region between the reflection surfaces, while “out”, “outward”, and “external” refer to positions, directions, and other items outside or away from the light-transmissive region. In general, it should be understood that the above directional orientation is arbitrary and only for ease of description, and that an optical cavity may have any appropriate orientation.

The above directional orientation does not in general apply to angle of incidence of input light. Transmissive cavities can typically operate in response to incident light that is not perpendicular to entry surfaces or reflection surfaces. Light incident on a transmissive cavity's entry surface at any angle is reflected multiple times within the cavity, producing transmission modes in accordance with the cavity's geometry. But transmission modes are affected by angle of incidence: Depending on the type of cavity and the angle of incidence, modes can be blue shifted or red shifted in comparison to perpendicular incidence; if all light enters a cavity at approximately the same angle, performance is affected only by the shifting of modes and modes are not also broadened, but performance is reduced if a cavity receives incident light distributed across a large angular range because transmission mode structure is then averaged over multiple angles.

Analyte is “present in”, “positioned in”, “contained in”, or simply “in” an optical cavity when the analyte is in all or some part of the cavity's light-transmissive region. An optical cavity provides “analyte-affected output light” if the optical cavity's output light is different in some way when analyte is present in the cavity than when analyte is absent, with the difference being due to the analyte's optical characteristics.

More generally, a cavity “includes a region” if the region is all or some part of the cavity's light-transmissive region. A region has a “changeable optical characteristic” if the region as a whole can be characterized as having the same value for the optical characteristic and if the value varies as a function of time; for example, a region has a “changeable optical absorption characteristic” if the region can be characterized by a single value for optical absorption and if that value fluctuates or otherwise varies over time. One way in which a region of a cavity can have a changeable optical characteristic is for the region to contain, in succession, a series of different analytes that have different optical characteristics affecting the cavity's output light, but there are many other possible ways in which a region could have a changeable optical characteristic with or without change in its contents.

As shown in FIG. 1, optical cavity 20 can include analyte 22 or region 24. In addition, cavity 20 has a set of one or more modes in which it provides output light, illustrated by solid-line curve 26 in the graph below cavity 20, which includes an “intensity function” for each of three modes of cavity 20, meaning that output light from each mode can be represented as a function, such as of photon energy or, in some implementations, of position.

An intensity function can have any of a wide variety of shapes and features, but a shape that frequently arises in transmission modes is the “peak”, a shape characterized by a maximum value from which a curve for the function slopes steeply downward. Peaks have various features, including “central energy”, applicable where intensity is a function of photon energy and meaning the photon energy at which the peak's maximum occurs; “maximum intensity” or simply “maximum” or “amplitude”, meaning the intensity value at the peak's maximum, whether measured as an absolute intensity or relative to another feature, such as a nearby minimum value; “contrast”, meaning a value indicating relationship between magnitudes of the peak's maximum intensity and one or more nearby minima of the transmission intensity function; and “intermediate intensity width”, meaning the width of the peak at an intensity somewhere between its maximum and nearby minima, such as a full width half maximum (FWHM). In general, values indicating these features can be obtained in various ways. For example, various numerators and denominators can be used in ratios computed to obtain values for contrast, including the following: If the numerator is a measured maximum intensity, then the denominator can be a minimum intensity near the peak or a well-defined non-minimum point of the transmission intensity function, such as a point where intensity if 50% or 1/e of the difference between maximum and minimum intensities. Further, the denominator can be the average of two nearby minima (or the other well-defined non-minimum points) such as the ones just left and right of the peak, the intensities at one or more nearby reflection mode maxima, and so forth.

Information about analyte 22 or region 24, such as an optical characteristic, can be encoded in a mode's intensity function, such as by changing its central energy or changing its amplitude, its contrast, or its FWHM, as indicated by dashed-line curve 28 in the graph: Central energies of the intensity functions for the first, second, and third modes are illustratively shifted from curve 26 to curve 28, such as by a change in refractive index; similarly, amplitudes, contrasts, and FWHMs of the intensity functions of the second and third modes are changed from curve 26 to curve 28, such as by changes in absorption spectrum.

The output light from optical cavity 20 can be received and photosensed by photosensing component 14. The dashed line from optical cavity component 12 to photosensing component 14 in FIG. 1 indicates, however, that optical cavity component 12 might be outside system 10; in other words, system 10 could receive output light from an external optical cavity, i.e. a cavity outside system 10, with photosensing component 14 receiving and photosensing the external optical cavity's output light. Furthermore, information about an optical characteristic or about an analyte or a region in or related somehow to an optical cavity internal or external to system 10 could be encoded in the intensity functions of an optical cavity's modes in various other ways besides the specific setup illustrated in FIG. 1; nevertheless, system 10 could obtain the information from the cavity's output light.

Photosensing component 14 obtains electrical signals that depend on an optical characteristic, such as of analyte 22, region 24, or another analyte or region in or related to optical cavity 20. As used herein, an “electrical signal” could be any signal capable of being electrically transferred from one component to another, whether by conductive, capacitive, or inductive coupling or any combination of types of coupling; once electrical signals have been obtained, of course, they can be stored in an appropriate storage component or converted or transduced to any other suitable form, including different types of electrical signals or electrostatic, magnetic, electromagnetic, mechanical, or other forms, for transfer or storage of information or for subsequent operations, as appropriate. An electrical signal “depends on” or “results from” an optical characteristic if the signal has some characteristic, whether digital or analog, that is determined by a value of the optical characteristic.

Photosensing component 14 could be implemented in many different ways, such as with a photosensing IC, as described in co-pending U.S. patent application Ser. No. 11/702,250, entitled “Photosensing Optical Cavity Output Light” and incorporated by reference herein in its entirety. The implementation in FIG. 1 might, however, alternatively be implemented with photosensing components that do not include photosensing ICs.

In the example in FIG. 1, electrical signals from photosensing component 14 are used by information obtaining component 16 to obtain information, such as about analyte 22, region 24, another analyte or region in or related to cavity 20, or an optical characteristic of analyte 22, region 24, another analyte or region, or the whole of cavity 20. FIG. 1 therefore illustrates a way of using a photosensing component to obtain information from an optical cavity's output light, such as information about an analyte, a region, or an optical characteristic such as refractive index or absorption. Various examples of types of information that could be obtained are mentioned herein, including not only measurements, spectra, derivatives, and so forth, but also “information about presence” of an analyte, which refers herein to any information about whether the analyte is present, such as in a sample, or in what amount, density, concentration, or other quantitative measure the analyte is present.

As an alternative to simply providing such information, such as in the form of data for storage or for use in subsequent operations of system 10 or for transfer to external components, information obtaining component 16 can also optionally adjust one or more optical characteristic values. For example, measurements with respect to a medium that is also present in cavity 20 can be used to adjust measurements with respect to analyte 22. Region 24 or another region within cavity 20 can, for example, contain a known reference medium, such as a fluid (e.g. liquid, gas, or aerosol) drawn from the same reservoir as fluid in which analyte 22 is carried through cavity 20 or, in cases where analyte 22 is in a bodily fluid, a reference fluid with a known concentration. Photosensed quantities indicating an optical characteristic of the reference medium can be compared with quantities obtained for analyte 22 in order to extract meaningful data such as magnitude or sign of a difference between photosensed quantities. Such reference-based adjustment techniques can be especially useful where both analyte 22 and the reference medium are subject to environmental variations such as temperature changes, because optical characteristics of both may undergo similar changes due to a given environmental change, leaving comparison results approximately constant; in effect, comparison with a reference can compensate for or remove effects of environmental changes.

The general features in FIG. 1 could be implemented in many ways, as exemplified by the various exemplary implementations described below. Also, photosensing component 14 could be implemented in many ways, including with various ICs that include devices with photosensitive surfaces that include discrete cells such as photosensor arrays, devices with continuous photosensitive surfaces such as PSDs, or any other type of photosensing components that can provide sensing results resulting from positions or intensities, such as of light spots. For example, photosensing component 16 could be implemented as a one-dimensional photosensor array with a coating as described below. In addition, photosensing component 16 could alternatively be implemented as a coated position-sensitive detector, as described in U.S. Patent Application Publication No. 2006/0039009, incorporated herein by reference in its entirety.

Photosensing components can provide electrical signals in various ways, including providing output currents from a PSD, integrating current or accumulating free charge carriers in cells at different positions of an array, and various other techniques. In each case, the electrical signals can be provided to other circuitry with appropriate techniques. While the output currents of a PSD or photodiode may in many cases be read out continuously, sensing results from cells of arrays are typically read out after sensing periods, such as with CCD or CMOS techniques.

Similarly, optical cavity component 12 and information obtaining component 16 could be implemented in various ways, some of which are described below. In addition, various components could be added to system 10, such as one or more optical components between components 12 and 14 to provide a suitable light distribution and minimize optical feedback between components. This could be achieved, for example, by incorporating an optical isolation component, an appropriate tilt, or optics between the components, or just by having a certain distance between the components that is larger than the coherence length of the light.

FIG. 2 illustrates optical cavity 100, an example of a “homogeneous optical cavity”, meaning a cavity whose light-transmissive region includes an extended part with substantially constant optical distance D between its reflection surfaces, sometimes referred to as its “homogeneous region”. The homogeneous region of cavity 100 illustratively includes substantially all of light-transmissive region 102 where it is between and partially bounded by light-reflective components 104 and 106, though partially and completely bounded homogeneous regions with various other shapes and arrangements are possible.

Inward-facing surfaces 110 and 112 of components 104 and 106, respectively, can be implemented, for example, as mirrors or other reflective components that closely approximate the reflection surfaces of cavity 100. The characteristics of components 104 and 106 and of any material or structure within region 102 are such that a measurement would indicate that at least a portion of light within region 102 is reflected more than once. A reflection direction in which light can be repeatedly reflected between the reflection surfaces is represented by bidirectional ray 114, while one of the possible lateral directions in an x-y plane approximately perpendicular to ray 114 is illustrated by an x-axis at the lower right.

FIG. 2 also illustrates two ways in which homogeneous optical cavities can operate to provide output light, represented schematically by arrows 116. In both operations, output light can be provided at an exit surface, illustratively outward-facing surface 120 of component 106, which may or may not be approximately parallel to the reflection surfaces.

In the first operation, optical cavity 100 operates as an emitting cavity, such as a laser cavity. Typically, an emitting cavity operates in response to stimulation of some type, represented schematically in FIG. 2 by stimulation arrow 122. Stimulation arrow 122 could, for example, represent electrical or optical stimulation.

In the second operation, optical cavity 100 operates as a transmissive cavity, such as a Fabry-Perot interferometer. A transmissive cavity operates in response to input light from one or more external light sources, represented in FIG. 2 by illumination arrows 124. Input light can be received at an entry surface, illustratively outward-facing surface 126 of component 104, which also may or may not be approximately parallel to the reflection surfaces. As noted above, a reflected portion of output light can be provided at the entry surface, as described in greater detail below.

FIG. 3 is an intensity-energy graph or “output spectrum” for optical cavity 100 when operated as a Fabry-Perot cavity such as an interferometer. Since photon energy is inversely proportional to wavelength, wavelength increases as one moves leftward along the horizontal axis, while the inverse of the wavelength (1/λ) increases as one moves rightward, as suggested by the labeling of points on the horizontal axis; it follow that energy and frequency would also increase to the right.

The graph in FIG. 3 includes a solid-line curve with peaks 130, 132, and 134, each of which is an “intensity-energy peak” or simply “intensity peak” that results from a respective transmission mode of cavity 100, illustratively the Kth, (K−1)th, and (K−2)th modes, and has an amplitude Imax, which could result from broadband illumination in the photon energy subranges of all the modes shown; such a curve is sometimes referred to herein as a “transmission spectrum”. FIG. 3 also includes part of dashed-line curve 136 that is the complement of the transmission spectrum, i.e. the intensity-energy curve for light that is reflected rather than transmitted by optical cavity 100; such a curve is sometimes referred to herein as a “reflection spectrum” and its reflection modes are broad and separated by narrow valleys rather than being narrow peaks separated by broad valleys like the transmission modes. The term “output modes” is sometimes used herein as a generic term that encompasses transmission modes and reflection modes.

The maxima of intensity-energy peaks 130, 132, and 134 (and the complementary minima between reflection bands) are spaced apart as a function of photon energy (illustratively wavelength), and the difference between the central energy of adjacent transmission mode peaks is referred to as “free spectral range” or “FSR”. FSR can be treated as the bandwidth over which adjacent intensity-energy peaks do not overlap, while the full width half maximum (FWHM) of the peaks can be treated as the minimum resolvable bandwidth. FSR, FWHM, and their ratio are all sometimes treated as figures of merit in designing a Fabry-Perot cavity.

The wavelength λ of each intensity-energy peak can be obtained from the equation λ(k)=2nD/k, where n is the refractive index of the cavity and k is a non-zero integer. Therefore, if refractive index of the cavity changes, λ(k) also changes for a given value of k, so that if a peak's central energy changes, as indicated by Δλ+ and Δλ− for peak 134, the change provides information about refractive index change. Similarly, the intensity of the peaks depends on absorption in the cavity, so that if the intensity of a peak departs from Imax, as indicated by ΔI+ and ΔI− for peak 134, the change provides information about absorption change.

FIG. 4 illustrates graded optical cavity 150, an example of an “inhomogeneous optical cavity”, meaning a cavity that does not meet the above definition of a homogeneous optical cavity. Because of the similarities between cavities 150 and 100, parts and components of cavity 150 that are substantially the same as those in FIG. 2 are labeled with the same reference numbers. In cavity 150, however, region 152 is not homogeneous, but rather has “laterally varying optical distance” between reflective surfaces, meaning that the optical distance varies in one or more lateral directions; in the illustrated example, the optical distance illustratively increases linearly from D(0) at one end of cavity 150 (x=0) to D(Xmax) at the opposite end (x=Xmax), but optical distance between reflective surfaces in an inhomogeneous optical cavity could vary laterally in any appropriate way, and need not vary monotonically, linearly, or with any other type of uniformity.

Because of its linearly varying optical distance or thickness, cavity 150 can operate as a linearly variable optical filter (LVF), a type of transmissive cavity. This capability is illustrated by the function T(x), a “laterally varying energy output function”, meaning that photon energies of output light depend on lateral position; in this case, the function relates output photon energy (in response to input light represented by illumination arrows 124) to lateral position on exit surface 120. For an LVF, the simple relationship λ(x)=T(x)=d′x+λ(0) can hold, where d′ is a constant that depends on gradient of optical thickness and can be graphically represented by the constant slope (λ(X2)−λ(X1))/(X2−X1)) of position-wavelength graph 154 at right in FIG. 4.

In general, the characteristics of output light at each position on surface 120 can be a function of parameters other than optical thickness, including, for example, photon energy and incident direction of input light 124 received at counterpart positions on surface 126. In particular, the output light may depend on whether the input light is narrow band, broad band, or multi-modal, as can result from a set of transmission or reflection modes. Narrow band or multi-modal illumination of an LVF, for example, can produce one or several output light spots, respectively.

The graphs at right in FIG. 4 also illustrate intensity-energy peaks 160 and 162 that would result if cavity 150 were illuminated by narrow band input light with central energy of λ(X1) and λ(X2), respectively, and, in response, operated as an LVF as described above. At position X1, for example, T(X1) results in transmission of output light represented by arrow 164, within a photon energy subrange characterized by central energy λ(X1); at position X2, T(X2) results in transmission of output light represented by arrow 166, within a photon energy subrange characterized by central energy λ(X2); for the illustrated laterally varying energy output function, if X1≠X2 and the difference between X2 and X1 is sufficient, then T(X1)≠T(X2), and λ(X1)≠λ(X2). On the other hand, for relatively small regions of output surface 120, cavity 150 might in some cases operate locally as a homogeneous cavity with transmission modes as illustrated in FIG. 3. It follows that parameters applicable to transmission modes are sometimes also useful for intensity-energy peaks from inhomogeneous cavities; in particular, information about changes in refractive index and absorption can sometimes be provided through changes in intensity-energy peaks in ways shown in FIG. 3.

Various techniques can be used to produce laterally varying energy distributions with inhomogeneous optical cavities having laterally varying optical thicknesses and, even with homogeneous optical cavities, with angled illumination from a point light source rather than perpendicular illumination; several possible techniques are described in co-pending U.S. patent application Ser. No. 11/316,438, entitled “Photosensing Throughout Energy Range and in Subranges” and incorporated herein by reference in its entirety.

More generally, an inhomogeneous optical cavity can have any appropriate laterally varying energy output function, including functions that are nonlinear or nonuniform in other ways. Some of the below-described implementations, for example, involve functions that are affected by presence of an analyte in an optical cavity. As with homogeneous cavities, an inhomogeneous cavity's light-transmissive region can be completely between and partially bounded by light-reflective components as in FIG. 4, but partially and completely bounded light-transmissive regions with various other shapes and arrangements are possible.

FIG. 5 is an intensity-position graph for optical cavity 150 when operated as a Fabry-Perot cavity such as an interferometer. FIG. 5 is similar to FIG. 3, and the peaks illustratively have maximum amplitude Imax as in FIG. 3 and their central energies and amplitudes (and FWHMs) could be affected as shown for peak 134 in FIG. 3; but the x-axis in FIG. 5 represents position in the x-direction in FIG. 4 rather than photon energy.

In the example shown in FIG. 5, cavity 150 is illuminated at P(P≧2) photon energies ranging from λmin to λmax, resulting in a series of output modes (illustratively transmission modes) for each photon energy λ(p) of illumination at those positions on the x-axis where the condition λ(p)=2n*D(x)/k is satisfied for integer values of k. The first transmission mode shown for λmin is peak 170 at x=Xmin(1) and for λmax is peak 172 at x=Xmax(1). The second transmission mode shown for λmin is peak 174 at x=Xmin(2) and for λmax is peak 176 at x=Xmax(2). The third transmission mode shown for λmin is peak 178 at x=Xmin(3), and so forth.

In the example of FIG. 5, transmission modes are sufficiently separated along the x-axis to prevent interference between adjacent transmission modes. As can be seen, Xmin(2) is sufficiently greater than Xmax(1) that peaks 172 and 174 do not interfere, and Xmin(3) is similarly sufficiently greater than Xmax(2) that peaks 176 and 178 do not interfere. If instead the first transmission mode of λmax were peak 180 due to an increase from Xmax(1) to Xmax(error), as indicated by arrow 182, interference between peaks 180 and 174 would begin to occur; as the first transmission mode of λmax increased further, loss of information would occur due to ambiguity between peak 180 and peak 174. Problems of this type can be avoided by coordination of photon energy range with cavity parameters; for example, cavity thickness D can be sufficiently small that only one output mode occurs over the range from λmin to λmax. The free spatial range (FSR) between the modes in a particular wavelength range can also be increased by reducing the tilt of the inhomogeneous (graded) cavity.

FIG. 6 shows a setup in which optical cavity structure 190 receives input light represented by arrows 192 through beam splitter 194. Optical cavity structure 190 can include a transmissive cavity implemented as in any of the ways described in relation to FIGS. 2-5 or in any other suitable way. In response to the input light, the cavity provides a transmitted portion of output light represented by arrows 196 and a reflected portion of output light represented by arrows 198. The use of beam splitter 194 is merely illustrative of ways in which input light and reflected light could be separated; for example, input light could be incident upon an entry surface at a sufficiently large angle from the normal that reflected light is separated from input light, though the non-perpendicular angle of incidence reduces performance of the optical cavity.

As suggested above in relation to FIG. 3, refractive index changes in the optical cavity will cause the same shift in both transmitted and reflected modes, while absorption in the optical cavity will similarly cause decreased amplitude (and contrast, as discussed below) and increased FWHM in both portions, with the effect of absorption typically varying as a function of photon energy; a curve showing absorption as a function of photon energy is sometimes referred to herein as an “absorption spectrum”.

FIG. 7 shows system 200, an exemplary implementation of system 100 in FIG. 1. System 200 includes optical cavity structure 202, a structure that can include one or more optical cavities with features described above. In system 200, at least one of the optical cavities in structure 202, represented schematically by cavity 204, can contain an analyte, illustratively being provided to cavity 204. The presence of analyte in cavity 204 affects the output light provided by structure 202, and the analyte-affected output light, represented by arrow 206, can then be photosensed within detector 210. For example, detector 210 may include a photosensing component with one or more photosensitive surfaces at which lateral variation of light is detected, such as after the light passes through an LVF. The sensing results from detector 210 can be provided to other components within system 200 or to external components, as represented by arrow 212.

Although cavity 204 can be any suitable type of homogeneous or inhomogeneous optical cavity, including an emitting cavity or a transmissive cavity, FIG. 7 illustratively shows one or more light sources 220 that can be included within system 200 to illuminate one or more optical cavities. As represented by arrow 222, structure 202 receives input light from light sources 220. If optical cavity 204 is illuminated as shown, the analyte-affected output light represented by arrow 206 could include one or both of transmitted and reflected light.

FIG. 8 illustrates electrical components that can be used in implementing system 200 as in FIG. 7. System 200 illustratively includes central processing unit (CPU) 240 connected to various components through bus 242, but a wide variety of other architectures could be employed, including any appropriate combination of hardware and software, as well as specialized hardware components such as application specific integrated circuits (ASICs) for one or more of the illustrated components or in place of a software component executed by CPU 240.

System 200 also includes component input/output (I/O) component 244, memory 246, integrated circuit input/output (IC I/O) 248, and external I/O 249, all connected to bus 242. System 200 can include various other components (not shown) connected to bus 242. In addition to connections through external I/O 249 by which signals can be provided to and received from external devices, bus 242 can also be connected directly to components outside of system 200.

Component I/O 244 permits CPU 240 to communicate with certain components of system 200, illustratively including illumination control 250, cavity control 252, and analyte control 254. For interactive applications, component I/O 244 could also be connected to a suitable user interface, such as a monitor and keyboard (not shown). In the exemplary implementation in FIG. 7, illumination control 250 can include light sources 220 (FIG. 7) and circuitry for controlling them; cavity control 252 can include electrodes or other components that can be operated to control cavity 204 and other cavities and can also include circuitry connected to those components; and analyte control 254 can similarly include fluidic devices or other components that can operate to transfer analyte into, through, or out of cavity 204 or other cavities or to produce relative movement between analyte and an array or a cavity, and can also include circuitry connected to those devices and components.

In the illustrated implementation of system 200, IC I/O 248 is a similar I/O component that permits CPU 240 to communicate with one or more ICs, such as in detector 210 in FIG. 5. M ICs are illustrated by a series from IC(0) 260 to IC(M−1) 262, including IC(m) 264 with a photosensor array 266.

Memory 246 illustratively includes program memory 270 and data memory 272, although instructions for execution by CPU 240 and data access during execution of instructions could be provided in any suitable way, including through external devices or components. The routines stored in program memory 270 illustratively include analyte information routine 274. In addition, program memory 270 could store various additional routines and also subroutines (not shown) that CPU 240 could call in executing routine 274. Similarly, the data in data memory 272 illustratively include calibration data 276, but could include various additional items of data and data structures accessed by CPU 240.

In executing routine 274, CPU 240 can provide signals to cavity control 252 and to analyte control 254 so that an analyte is present in cavity 204, for example, with the analyte having optical characteristics that affect output light from cavity 204. CPU 240 can also provide signals to illumination control 250 so that cavity 204 is appropriately illuminated to provide analyte-affected output light. CPU 240 can also provide signals to each of ICs 260 through 262 to obtain sensing results that include information about the analyte in cavity 204. In an implementation with a position-sensitive detector (PSD), CPU 240 could instead provide whatever signals are necessary to obtain photosensed quantities from the PSD; for example, CPU 240 could control circuitry to connect output currents from the PSD to a differential amplifier.

FIG. 9 illustrates one example of how analyte information routine 274 could be implemented in a system like system 200 in FIGS. 7 and 8. The routine in FIG. 9 could be implemented for single objects moving along paths through cavities past arrays; for spaced multiple objects moving along paths through cavities past arrays; or for continuous streams of objects, such as small volumes of fluid, moving along paths through cavities past arrays, in each case subject to appropriate constraints.

Examples of objects that could occur in implementations as described herein include droplets, bubbles, small volumes of fluid, single molecules, agglomerated molecules, molecule clusters, biological cells, viruses, bacteria, proteins, DNA, microparticles, nanoparticles, and emulsions. A droplet or small volume of fluid may, for example, include atoms, molecules or other particles that affect refractive index, absorption, or other optical characteristics. An object “travels” or is caused “to travel” if the object moves through a succession of positions. For example, the object could be conveyed in a fluid, such as a liquid, gas, or aerosol, in which case the object may be referred to as being “carried by the fluid.”

The term “path” is used herein to refer to a substantially continuous series of positions through which an object may travel. A path is “through a cavity” if an object following the path passes through part of the cavity. A photosensing component, such as an array or PSD, is “positioned along” or “along” a path through a cavity if the component is positioned near the cavity in such a way that, when an object following the path affects output light from the cavity, the photosensing component can obtain sensing results that include information about how the object is affecting the output light; it is not necessary, however, that the photosensing component be immediately against or adjacent to an external surface of the cavity that includes the path—there could, for example, be another optical cavity or other optical component between them, such as an LVF. An object following a path in a case where an array is along the path in any of these ways can be said to move “past the array”.

The routine in FIG. 9 follows a general strategy of performing a series of readout operations, after which information is combined and provided. It would also be possible to provide the information from each readout operation immediately or to provide information both immediately after each readout operation and also after a series of readout operations.

When CPU 240 executes the operation in box 300, it performs a pre-sensing readout. The purpose is to obtain information necessary to later perform a sensing readout. The information could be obtained in the ways described in co-pending U.S. patent application Ser. No. 11/315,992, entitled “Sensing Photons from Objects in Channels” and incorporated herein by reference in its entirety.

Using the information from box 300, CPU 240 could obtain information about each object and determine an appropriate sensing period for each object, in the operation in box 302. For example, CPU 240 could perform calculations to determine whether one or more objects are present, the position of each object, and the speed of each object. Using this information and taking into account previously calculated sensing periods for the same objects, if any, CPU 240 can also determine an appropriate sensing period to be used during sensing readout; in general, the sensing period must provide an integration time shorter than the time necessary for an object to pass each cell in an array. Each object can therefore have a unique sensing period.

The operation in box 302 can also include providing any necessary signals through component I/O 244 to adjust movement of objects, such as by adjusting fluid speed; to adjust illumination or stimulation of the optical cavity; or to adjust characteristics of the optical cavity, such as by adjusting optical distances between light-reflective components or by adjusting temperature or another operating parameter of the cavity. These signals could include any appropriate combination of signals to illumination control 250, cavity control 252, and analyte control 254, two or more of which could be concurrently receive signals so that more than one adjustment is made at the same time, such as system temperature and also illumination. CPU 240 could provide such signals based in part on information it obtains from optical cavity output light, such as through techniques as described below.

CPU 240 can then perform sensing readout on a cavity's output light, in box 304. This operation includes providing signals through IC I/O 248 so that photons are photosensed cumulatively during the sensing period obtained in box 302, and may also include signals to peripheral circuitry on an IC so that analog quantities photosensed by cells are adjusted based on reference values. After adjustment, if any, analog quantities can be converted to digital signals for readout. The operation in box 304 can be implemented in whatever manner is appropriate for a given IC, whether a CCD or CMOS implementation, and regardless of whether readout is purely serial or is also parallel.

Sensing results obtained in box 304 can include information about objects and analytes in them. Since an analyte's or object's optical characteristics can affect the output light provided in a mode of an optical cavity, such as in the ways described above in relation to FIGS. 1, 3, and 5, information about the analyte's optical characteristics is present in the cavity's output light, encoded in intensity functions of one or more modes. Detector 210 as in FIG. 7 can include, for example, a laterally varying transmission structure, so that an intensity-energy peak in the analyte-affected output light has a respective light spot on a photosensing IC in detector 210. Therefore, the sensing results can include information about at least one of position and intensity of a light spot and, accordingly, about the respective intensity-energy peak and about the optical characteristics as shown. If the output light from the cavity includes two or more intensity-energy peaks, their respective light spots can be tracked separately as described below.

The photosensed quantities read out in box 304 can also be digitally adjusted by CPU 240 before being stored for each light spot, in box 306. The digital adjustment can include adjusting quantities photosensed by cells based on reference quantities or based on calibration data 276 (FIG. 8), and can also include any necessary adjustments due to differences in sensing periods or other factors; calibration-based techniques that can be used are described in co-pending U.S. patent application Ser. No. 11/633,302, entitled “Position-based Response to Light” and incorporated herein by reference in its entirety.

The digital adjustment in box 306 and the analog adjustment, if any, in box 304 can also employ reference cell-based adjustment techniques described in co-pending U.S. patent application Ser. No. 11/316,438, entitled “Photosensing Throughout Energy Range and in Subranges” and incorporated herein by reference in its entirety; such reference cell-based adjustment techniques may be especially useful for intensity referencing in tracking an object's position, and can, in general, be performed in relation both to measurements of refractive index and also of absorption. In particular, such adjustments can be used to overcome problems with inhomogeneous illumination, but such techniques may be difficult to implement successfully in system 200 because external inhomogeneities that affect output light, such as in illumination or in stable or time-varying absorption by particles between light sources 220 and optical cavity 204, are not readily distinguishable from absorption within cavity 204. In other words, adjustment based on reference cells may remove desired information about absorption changes inside cavity 204.

To avoid this and other such problems, the operation in box 306 or a subsequent operation can make an alternative data manipulation or adjustment to obtain “cavity-only absorption data”, an expression that refers herein to values or other data in which information about absorption in cavity 204 is preserved while information is reduced about features exterior to cavity 204 such as inhomogeneities in illumination and external absorption; such information can, for example, be reduced so that it is indistinguishable from other noise in the cavity-only absorption data. Contrast-based data provide examples of cavity-only absorption data. For each object, analyte, or region for which absorption information is obtained, calculating contrast-based values or other data can remove effects other than those from absorption coefficient inside cavity 204, influences such as external perturbations, disturbances, or inhomogeneities. As a result, measurements of absorption can have a higher signal to noise ratio. Also, information can be obtained that is selectively sensitive to absorption changes inside cavity 204. Since it does not require reference cells or reference measurements, contrast-based data can improve efficiency and feasibility, such as by reducing the number of elements required in photosensing arrays and, accordingly, power consumption by arrays.

Contrast-based data can be obtained, for example, by obtaining a value for contrast C, which is defined in general as the ratio between maxima and minima of a cavity's transmission intensity function and specifically, for a Fabry-Perot cavity, by the following equation:

${C = {\frac{T\;\max}{T\left( {\delta = \frac{\pi}{2}} \right)} = {1 + \frac{4\; F^{2}}{\pi^{2}}}}},$ where F is finesse and Tmax is maximum transmittance for the cavity's modes; these and other variables in the equation for C are described in greater detail below. As can be seen, C is only dependent on properties of a Fabry-Perot cavity. It is not influenced by intensity of incident light, but is highly sensitive to absorption coefficient inside the cavity since absorption inside the cavity affects the cavity's finesse. Although finesse can in turn be calculated from cavity parameters, e.g. from reflectivities and absorption as in an equation set forth below, it can also be visualized, because a cavity with higher finesse will have sharper transmission peaks and lower minima between peaks.

It follows from the above that contrast-based data can be obtained in box 306 by first obtaining a mode's maximum intensity and the adjacent minima (or another intensity that provides information about minimum intensity, such as an intermediate intensity at 50% or 1/e of the difference between maximum and minimum intensities) or other appropriate values, such as based on width of transmission mode or on positions of maxima of reflection modes; in general, maxima and minima can be similarly obtained for intensity-energy functions or for intensity-position functions. These values can then be used to obtain the mode's value for C. In obtaining contrast-based data in most cases, there is an ambiguity in which values should be used in computing a contrast ratio. For example, a maximum is usually between two adjacent minima (and, accordingly, two intermediate intensity points). One can therefore avoid error that might result if only one minimum value is used by taking the ratio of twice the maximum to the sum of the adjacent minima (or, accordingly, the two intermediate intensity points of one peak). The value for C can itself be used in further operations or, alternatively, another value that depends on absorption coefficient can then be obtained from the value for C, such as based on equations discussed in greater detail below.

Contrast-based data provide especially useful examples of cavity-only absorption data, but there are other examples, including FWHM-based values or other data, some of which are discussed in greater detail below. The relationship between FWHM and finesse F can be understood from the following equation:

${{FWHM} = {\frac{c_{0}}{\pi\;{nd}}{\arcsin\left( \frac{\pi}{2F} \right)}}},$ in which c₀ refers to the speed of light, n to the refractive index, and d to the width of the cavity. As can be seen by comparing the two equations, both FWHM and contrast include information about finesse, though they depend on finesse in different ways and are therefore sometimes useful in different contexts.

More generally, other adjustment techniques that can be used, such as in box 306, are described in co-pending U.S. patent application Ser. No. 11/702,329, entitled “Implanting Optical Cavity Structures” and in co-pending U.S. patent application Ser. No. 11/702,325, entitled “Containing Analyte In Optical Cavity Structures”, both of which are incorporated herein by reference in their entireties.

Orientation of components can result in non-perpendicular incidence of input light on optical cavities, such as if an operation in one of boxes 302 and 304 changes the tilt of the entry surface at which a cavity receives incident light. Unless all output light is incident on one position of the detector component or the detector component has only a single large area as with some PSDs, adjustments can be made to correct for non-perpendicular incidence of input light: For example, if the light source component emits light from a point source at many different angles that are accordingly transmitted through the cavities at various angles, the detector component's photosensitive surface receives the output light at many different angles, but each cell of a photosensor array would receive only a very small angular distribution; therefore, if the angle could be known, as would be the case in a fixed geometry but may not be the case in FIG. 7, the angle-induced variation can be easily corrected.

The position and speed information about each object from box 302 can be used by the operation in box 306 to determine which photosensed quantities result from effects of each object. Similar techniques can be used to determine which photosensed quantities result from each mode's light spot when a cavity's output light includes two or more modes.

For homogeneous analyte in cavity 204 or for stationary or slow-moving objects in cavity 204, lock-in techniques could be applied to further improve signal to noise ratio, such as by modifying operations in boxes 302, 304, and 306 in FIG. 9. For example, illumination from light sources 220 can be modulated in order to modulate output light from cavity 204. The applicable modulation frequencies would be constrained by the readout frequency achievable by detector 210. In implementations where it is not possible to directly record a correlation signal, another type of reference could be used, such as an empty channel in a fluidic structure, a channel with a reference medium, or an uncoated reference cell in a photosensing array with coated cells to sense photon energy subranges.

In performing the operations in boxes 304 and 306, CPU 240 can employ data structures (not shown) stored in memory 246. For example, one data structure can store each object's previously calculated position and speed, which can then be used in performing subsequent calculations to identify effects of the same object; similarly, each object's data structure can also include each light spot's identifying information and the object's effect on the identified light spot, which can similarly be used in subsequent calculations. Also, a readout data structure can be employed to hold all of the adjusted quantity information about each object.

The operation in box 306 can update the readout data structure each time it obtains additional information about the same object. In an implementation as in FIG. 8, the operations in boxes 300, 302, 304, and 306 can be performed separately for each of ICs 260 through 262. Further, as suggested by the dashed line from box 306 to box 300, the same operations can be performed repeatedly for each of the ICs. If each object can be correctly identified throughout its travel along a path through cavity 204, the readout data structure can be used to hold all of the information obtained from all ICs. Between consecutive executions of the operations in boxes 300, 302, 304, and 306, the effects of each object may move only a few cells along the path, and consecutive objects must be sufficiently separated to avoid confusion. For example, each object may be a few μm in diameter, each cell may have a length along the path of between 10 and 20 μm, and consecutive objects may be two or three cell lengths apart. For larger objects or for cells of different sizes, the spacing between consecutive objects can be adjusted appropriately.

Various modifications could be made in the implementation of FIG. 9. For example, rather than being spaced apart, objects could be closer together. Even if several objects are having overlapping effects on a light spot, it may be possible to perform computational algorithms to separate the effects of the objects. Similarly, if objects are very close to each other but positioned along different cells, an optical structure between the path of the objects and detector 210 could ensure that photons affected by different objects travel to different cells; in this way, a continuous stream of objects could be measured. Furthermore, techniques as described above could be applied to a continuous fluidic stream without distinguishable objects in it, in which case the analyte-affected output light from optical cavity 204 would be determined by optical characteristics of concentrations of molecules in each position in the stream rather than by optical characteristics of distinguishable objects. In effect, the stream would be divided into imaginary small volumes, each of which would be an object analyzed as described above, allowing for continuous monitoring of how the output light from the fluid changes with time, such as due to changing composition of the fluid.

As the operations in boxes 300, 302, 304, and 306 are repeated while an object travels along a path past detector 210, more and more information is obtained, especially where a cavity's output light has more than one light spot, with each light spot having a respective position on the array. When the object has passed the whole array, information about the analyte it contains can be recomposed from the stored fractions.

Upon completion of any suitable amount of information gathering in boxes 300, 302, 304, and 306, CPU 240 can perform the operation in box 310 to provide analyte information, such as in the form of data for another routine or as output through external I/O 249. As shown, this operation can include combining the sensed quantities for each object so that analyte information for the object can be provided, such as in the form of an absorption spectrum, a value for the analyte's refractive index, or some other data structure.

Many possible uses exist for analyte information as obtained in box 310, and operations like those in FIG. 9 could be implemented with a wide variety of existing technologies; analyte information could be used, for example, to distinguish objects, as described in detail in co-pending U.S. patent application Ser. No. 11/702,328, entitled “Distinguishing Objects” or to detect glucose in bodily fluids, such as with techniques described in co-pending U.S. patent application Ser. No. 11/702,329, entitled “Implanting Optical Cavity Structures”, both of which are incorporated herein by reference in their entireties. Furthermore, it is foreseeable that further uses of analyte information and technologies for implementing such operations will be developed in the future. In general, analyte information from box 310 can be used in any way whatsoever, including not only existing techniques but also techniques developed hereafter. The operations illustrated in FIG. 9 do not require any specific technology, such as for data storing or processing operation, and are compatible with any such technology that exists now or may be hereafter developed.

FIG. 10 shows device 350, which could be used in an implementation of system 200. Entry glass 352 and an exit glass (not shown) are of substantially the same size and shape, and their inward-facing surfaces have coatings or other structures that function as light-reflective components, reflecting light into a light-transmissive region between them to operate as an optical cavity. The two glasses are illustratively separated by spacers 354 and the light-transmissive region may also contain fluidic walls or other structures (not shown) that bound a duct or channel between inlet 356 and outlet 358; as a result, an analyte or a fluid carrying an analyte can enter the optical cavity from inlet 356, can be carried along a path through the optical cavity such as through a duct or channel, and can then exit from the optical cavity to outlet 358.

Over or on entry glass 352 is light source component 360, which can include one or more light sources such as lasers, LEDs, or super luminescence diode (SLDs) to illuminate the optical cavity. Photosensing array 362 is on the underside or below the exit glass, positioned along the analyte's path through the optical cavity. Light source component 360, array 362, and the optical cavity between them have characteristics such that the optical cavity responds to illumination from the light sources by providing analyte-affected output light that can be photosensed by array 362.

FIG. 11 shows a longitudinal cross-section of device 350, viewed along the line 11-11 in FIG. 10. In the illustrated cross-section, light sources 360 are providing light, represented by arrows 380, which passes through entry glass 352 and through entry light-reflective structure 382 before entering channel 384. Within channel 384, a moving fluid such as a liquid, gas, or aerosol, represented by arrows 390, carries an object 392. While object 392 is present in the optical cavity, its optical characteristics can affect light reflected within channel 384 between entry light-reflective structure 382 and exit light-reflective structure 394. As a result, analyte-affected output light exits through exit light-reflective structure 394 and is transmitted through exit glass 396 and then transmission structure 398 before being photosensed by array 362.

In general, object 392 can be a particle, droplet, or small volume of fluid that can be carried by a fluid or other appropriate substance and that includes an analyte to be analyzed. The term “object” is used herein in the general sense of any distinguishable thing that can have optical characteristics such as refractive index and absorption. More generally, any energy shifting or loss mechanism associated with a distinguishable thing within the cavity affects transmitted and reflected wavelength and intensity, and is therefore a type of optical characteristic as used herein, including, for example, scattering and reflection.

The terms “fluidic structure” and “channel” are used herein with related meanings: A “fluidic structure” is a structure that depends for its operation on fluid positioning or fluid flow, such as, for liquids or gases, in response to pressure or, for liquids, as a result of surface tension effects; a “channel” is any tube or other enclosed passage defined within a fluidic structure and through which fluid flows during operation. The direction in which fluid flows within a channel is sometimes referred to herein as a “flow direction.”

Transmission structure 398 can be an LVF implemented as described above in relation to FIG. 4 or can be any other appropriate transmission structure with a suitable laterally varying energy output function, so that incident light on array 362 similarly has a “laterally varying photon energy distribution” or simply a “laterally varying energy distribution”, meaning that photon energy of incident light varies as a function of lateral position. For example, transmission structure 398 can provide a laterally varying energy distribution on array 362 by transmitting, at each position along channel 384, only light in a respective narrow subrange of photon energies, with the respective subranges being different at different positions along channel 384. Therefore, for each position, a respective set of one or more cells of array 362 receives light only if the position's respective subrange includes or overlaps with a subrange in which the optical cavity is providing output light, such as the subrange of an intensity-energy peak as illustrated in FIG. 4.

A detector or other device or apparatus including both transmission structure 398 and array 362 could be implemented in a wide variety of ways, some of which are described in co-pending U.S. patent application Ser. No. 11/315,386, entitled “Sensing Photon Energies Emanating from Channels or Moving Objects,” and incorporated herein by reference in its entirety. For example, array 362 could have a photosensitive surface with an appropriate pixel- or cell-density and transmission structure 398 could be a coating over the photosensitive surface that operates as an LVF.

Array 362 could be implemented with any appropriate readout technique, such as CMOS or CCD readout, for which cell dimensions of 5-50 μm are currently typical, and smaller cell dimensions are foreseeable. Although array 362 could be a one-dimensional array with a line of cells parallel to the flow direction of arrows 390, implementation with a two-dimensional array could beneficially provide, at each position along the path of object 392, a set of two or more cells in a line perpendicular to the flow direction, with all the cells in the set concurrently photosensing incident light in the same photon energy subrange; sensing results from each set of cells could be used to average or otherwise combine and improve information obtained for a given transmission mode's output light.

Entry and exit light-reflective structures 382 and 394 operate as two parallel mirrors, with channel 384 being a light-transmission region between them, providing an optical cavity as described above. With appropriate parameters, the cavity can operate as a Fabry-Perot interferometer, and its transmission properties will be determined by the mirrors and the region between them: The mirrors affect FWHM of peaks of the cavity's transmission spectrum and their reflectivity also affects the quality of the stop-band, i.e. how much light is transmitted outside of transmission modes. Also, the refractive index and distance between structures 382 and 394 affect or determine the photon energies that are transmitted by the optical cavity.

Each of structures 382 and 394 can be implemented as a layered structure with alternating dielectric layers or with metal, deposited in either case on entry glass 352 and exit glass 396. Rather than glasses 352 and 396, the enclosing walls of channel 384 through which light enters and exits could instead be implemented with any other suitable light-transmissive components with inward-facing surfaces that are or can be made reflective, such as by fabrication of appropriate structures on them.

In an illustrative implementation, light source 360 illuminates the optical cavity homogeneously with a collimated light beam from a suitable light source, such as an LED, broadband laser, or superluminescence diode (SLD); suitable optical components can be used to spread a light beam to illuminate all of array 362, such as with spreading components as disclosed in copending U.S. patent application Ser. No. 11/315,387, entitled “Propagating Light to be Sensed” and incorporated herein by reference in its entirety. In other implementations, light source 360 could include or be replaced by an array of light sources, reducing or eliminating the need for spreading. For example, a single broadband light source like an LED or SLD could be replaced by an array of laser diodes (not shown) or narrow-band emitting LEDs (e.g. resonant cavity LEDs), each emitting at a respective wavelength; this approach could beneficially increase the interaction length between light and analyte in larger cavities in which interaction length is limited by a light source's coherence length. In addition, since different positions of transmission structure 398 transmit different photon energy subranges, each laser diode in the array could beneficially be positioned or oriented to illuminate a respective position at which transmission structure 398 transmits the diode's emission wavelength.

If object 392 is absent and fluid in channel 384 is homogeneous, device 350 can operate as a homogeneous optical cavity as described above in relation to FIGS. 2 and 3. The output light from the optical cavity can include one or more discrete transmission modes if the dimensions and refractive index of the optical cavity are appropriate. The presence of object 392, however, can change the refractive index and absorption of the optical cavity due to optical characteristics of object 392. For example, if object 392 has a certain absorption spectrum, it can affect the intensity amplitude Imax and the FWHM of each transmitted mode as illustrated in FIG. 3 and also its contrast C as described above; similarly, the refractive index of object 392 can affect photon energies of the modes as illustrated in FIG. 3. These are examples of “encoding information” about optical characteristics, an expression used herein to refer to any operation or combination of operations by which an optical cavity's output light is modified in a way that depends on optical characteristics, such as of object 392.

In response to output light from the optical cavity, array 362 can accordingly obtain sensing results that indicate changes in the central energy, intensity amplitude, FWHM, and contrast of each transmitted mode, providing information about object 392 and its effect on the refractive index and absorption in the optical cavity. The sensing results can then be used, such as by CPU 240 in executing analyte information routine 274 to “obtain information”, an expression used herein to refer to any operation or combination of operations performed on sensing results from photosensing an optical cavity's output light and that produce indications of information encoded in the output light; the indications could, for example, be electrical signals, data stored by an appropriate memory device, displayed information, and so forth. For example, sensing results that indicate intensity, FWHM (or other intermediate intensity width), contrast (e.g. Tmax/Tmin or other suitable value), or any other relevant measurable feature of each transmitted mode can be used to obtain data indicating an absorption value for a given photon energy such as the central wavelength of the mode; similarly, sensing results indicating central energy shift can be used to obtain data indicating a refractive index value for the optical cavity with object 392 present.

An alternative approach could encode information about optical characteristics in reflection modes of a Fabry-Perot cavity rather than in transmission modes. Sensing results from reflection modes could be used, for example, to obtain information about absorption spectra and refractive index dispersion. This approach could be beneficial in applications where improved readout sensitivity is desirable: Analyte could fill or otherwise be positioned within a slightly asymmetric Fabry-Perot cavity designed so that the cavity with analyte approximates a symmetric Fabry-Perot cavity, which would be true for a cavity of width w and absorption α if the second mirror's effective reflectivity Reff(2) is substantially equal to the first mirror's reflectivity R(1) as follows: Reff(2)=R(2)*exp(−2αw)=R(1)

In some implementations of system 200, object 392 would be a biological cell carried by liquid flowing through channel 384, and device 350 could be used to encode information about optical characteristics of a series of such cells and to obtain sensing results indicating the encoded information; information about the optical characteristics could then be obtained from the sensing results by CPU 240 and used in an appropriate way, such as for the purpose of distinguishing types of biological cells. In encoding and obtaining information about refractive index, for example, the information will result not only from a biological cell but also from the fluid or other medium that is carrying it and fills channel 384 around the cell. The resulting measured refractive index will therefore be a combination between that of the fluid and that of the biological cell. If the size of the cell is known, its actual refractive index could be determined from the measured refractive index; the size of the cell can be determined, for example, by using a Coulter counter and/or a light scattering unit, such as an MIE scattering device.

FIG. 12 shows two transmission spectra that illustrate how a change in refractive index shifts transmission peaks. The illustrated portion of the spectra includes six pairs of peaks near a wavelength of 1.0 μm. In each pair, the leftward peak was obtained with a refractive index of 1.30 while the rightward peak was obtained with a refractive index of 1.31. In both cases, the width w of the cavity operating as a Fabry-Perot interferometer was 10 μm. As can be seen, the FSR is approximately 37 nm, while the shift Δλ resulting from the refractive index change of 0.01 is approximately 8 nm. This is consistent with the following equations for the case of incident light parallel to the reflection direction:

$\begin{matrix} {{FSR} = {{\lambda(k)} - {\lambda\left( {k + 1} \right)}}} \\ {= {2{{nw}/{k\left( {k + 1} \right)}}}} \\ {\overset{k->\infty}{\approx}{{\left( {\lambda(k)} \right)^{2}/2}{nw}}} \end{matrix}$ and Δλ(k) = 2Δ nw/k.

In general, the first of these equations shows that FSR becomes smaller, and transmission peaks therefore become closer, as w increases. Also, a slight increase in n causes a slight increase in FSR. These effects, however, are not readily visible in FIG. 12.

In designing device 350 to encode information about optical absorption and to obtain sensing results indicating such information, several constraints must be taken into account—the desired absorption or interaction length; the desired volume of analyte; the required photon energy range and resolution for absorption spectra; the wavelength resolution of the detector that includes transmission structure 398 and array 362; and so forth. To reach a suitable compromise between these constraints, several parameters can be adjusted, including the width of the cavity, the reflectivity of the mirrors, size of array 162, properties of transmission structure 398, and possibly absorption within the cavity, though absorption is not easily adjusted.

Device 350 as in FIGS. 10 and 11 can also be used to encode information about a homogeneous analyte such as a liquid, gas, or aerosol, within channel 384 without the presence of object 392. For example, a single readout of sensing results from array 362 can provide information about the transmission spectrum of the homogeneous analyte. If the analyte changes on a relatively long time scale compared to transit time through device 350, sensing results read out at different times can indicate long-term changes of the transmission spectrum. For this approach, however, accurate measurements can only be obtained if the analyte present within channel 384 during a given readout is substantially homogeneous.

FIG. 13 illustrates graphically the effect an analyte can have on a Fabry-Perot interferometer's transmission spectrum. The cavity illustratively has a width w of 75 μm and a mirror reflectivity of 95%. Without analyte present in the cavity, each of the illustrated transmission modes transmits light to a normalized intensity amplitude of 1.0, as shown in the upper part of FIG. 13.

With the analyte present, in this case glucose in water, transmission of nearly all modes is decreased due to absorption, with the resulting peaks for the illustrated modes falling on curve 410 in the lower part of FIG. 13. Curve 410 can therefore indicate the absorption spectrum of the analyte, with the circles 412 serving as discrete sampling points of the absorption spectrum. In order to measure the absorption spectrum to a desired resolution, the cavity width w and other parameters must be chosen to obtain a sufficient number of sampling points.

FIG. 13 also suggests that increased glucose absorption dramatically reduces intensity of a mode because of the strongly enhanced interaction length that occurs within a cavity with highly reflective mirrors. This means that light bounces back and forth within the cavity many times before being transmitted. As described above, the increased analyte absorption also causes broadening of the modes. The larger the absorption, the smaller the mode's intensity and contrast and the larger the mode's FWHM (or other intermediate intensity width); the lower part of FIG. 13 does not fully show the change in FWHM that would occur. Additional details about effects of absorption are provided in co-pending U.S. patent application Ser. No. 11/702,363, entitled “Encoding Optical Cavity Output Light” and incorporated herein by reference in its entirety.

As suggested by arrows 390 in FIG. 11, object 392 can move at a relatively uniform speed along a path within channel 384. As a result, its effect on transmission modes of the optical cavity will also follow a path, allowing correlation between sensing results from array 362 and the position of object 392, such as with the techniques described in co-pending U.S. patent application Ser. No. 11/315,386, entitled “Sensing Photon Energies Emanating from Channels or Moving Objects” and incorporated herein by reference in its entirety. In effect, a series of cells in array 362 obtain sensing results that include information about optical characteristics of object 392. These sensing results can be used to obtain information as described herein.

In the specific example illustrated in FIG. 11, absorption spectroscopy could be performed, for example, by obtaining sensing results as object 392 moves through channel 384, using the sensing results to obtain actual absorption values of object 392 for each transmission mode based on biological cell size and flow velocity, and composing an absorption spectrum using the actual values obtained. This technique takes advantage of the motion of object 392 for improved detection, and also enables large integration times without losing throughput capacity. Highly sensitive optical absorption spectroscopy can be performed in this manner.

FIGS. 14-15 show device 440, an alternative implementation with features similar to those shown in FIGS. 10-11, but with multiple channels 450, 452, 454, 456, and 458 bounded by walls 460 and with a flow direction indicated by arrows 462. A single two-dimensional photosensing array 470 can obtain sensing results for all the channels, with sets of cells providing sensing results in the manner described above for two-dimensional arrays. Biological cells or other objects, represented by the shaded circles such as circle 472, can be correlated with their sensing results based on flow velocity, as described above.

FIG. 15 shows a cross-section of device 440 taken along the line 15-15 in FIG. 14. As in FIG. 11 above, light sources 480 could be implemented in any appropriate way to illuminate channels 450 through 458. Entry glass 482 could have entry light-reflective component 484 formed on its inward-facing surface as described above, and exit glass 494 (or another substrate that can carry a mirror) could have exit light-reflective component 492 formed on its inward-facing surface. Transmission structure 490 could be formed on array 470.

Transmission structure 490 could be implemented in any of several different ways to provide desired sensing results. For example, transmission structure 490 could be a layered structure, implemented with any of the techniques described in co-pending U.S. patent application Ser. No. 11/316,303, entitled “Obtaining Analyte Information” and incorporated herein by reference in its entirety.

In one exemplary implementation, transmission structure 490 could be an LVF that is graded in the x-direction shown in FIG. 14 but is homogeneous in the y-direction. In this case, array 470 would be sensitive to the same photon energy subrange in all of channels 450 through 458. Therefore, information about the same changes in refractive indices and absorption information could be obtained from all the channels, with parallel positions in the channels providing information about the same photon energy subranges. Since the subranges vary along each channel, information can be obtained for a number of different subranges or for an entire spectrum as a biological cell or other object is carried through a channel. In this case, all channels are identical and objects or analytes are characterized in the same manner independent of the channel through which they are passing.

In another exemplary implementation, transmission structure 490 could be an LVF that is graded in the y-direction in FIG. 14 but homogeneous in the x-direction. This arrangement could be obtained, for example, by rotating the previously described exemplary implementation through 90°. In this case, a set of two or more cells that extend in a line across a channel at a certain position will receive different photon energy subranges, so that the intensity ratio between cells in such a set will change as a biological cell or other object passes by while being carried through the channel. In this case, refractive index change of an object can be recorded as a function of time while it is moving along the channel, or multiple measurements or longer integration times (in the case of a homogeneous analyte) can be used to increase sensitivity. Note that in parallel channels different modes are used to determine refractive index.

In yet another exemplary implementation, transmission structure 490 could be graded in both the x-direction and the y-direction. This case would allow information to be obtained about different subranges in both of the ways described above.

In general, various referencing techniques could be used to measure optical characteristics such as absorption spectra and refractive index values by comparison to reference values obtained from the same optical cavity, such as with a known reference solution or other fluid. In the implementation in FIGS. 14 and 15, for example, every other channel, such as channels 452 and 456, could serve as a reference channel if it is empty or contains only a known homogeneous reference fluid, allowing more precise evaluation of absorption spectra and dispersion of the refractive index in channels 450, 454, and 458, such as by comparing measured analyte values with measured reference values; for example, to sense glucose concentration based on optical characteristics, the reference medium could be a known glucose concentration. Since reference medium and analyte are moving within the same environment or channel system this also allows compensation for external influences (like temperature, pressure, etc.) that may have a significant influence on optical properties.

FIG. 16 illustrates exemplary operations in producing a device like device 350 in FIGS. 10 and 11 or device 440 in FIGS. 14 and 15. In particular, the operations in FIG. 16 make it possible to produce apparatus in which information about optical characteristics of an analyte can be encoded and sensing results indicating the information about the optical characteristics can be obtained.

The operation in box 520 in FIG. 16 produces entry and exit partial optical cavity structures. This operation can include producing entry light-reflective structure 382 on entry glass 352 and also producing exit light-reflective structure 394 on exit glass 396, both as in FIG. 11. Similarly, this operation can include producing entry light-reflective component 484 on entry glass 482 and also producing transmission structure 490 and exit light-reflective light component 492 on photosensing array 470 as in FIG. 15. This operation can also include producing a patterned layer of SU-8 or polydimethylsiloxane (PDMS) on one or both of the light-reflective structures, such as with techniques described in co-pending U.S. patent application Ser. No. 11/315,992, entitled “Sensing Photons from Objects in Channels” and incorporated herein by reference in its entirety. This patterned layer could include structures such as spacers 354 in FIG. 10 and walls 460 in FIGS. 14 and 15. If appropriate, an anti-adhesive coating can be applied to interior channel surfaces, such as by dip-coating polyethylene glycol (PEG) or by providing a coating of parylene C or vapor deposited tetraglyme.

The operation in box 522 then attaches the entry and exit partial structures, with attached fluidic components to position analyte in the resulting optical cavity. The operation in box 522 can include forming a suitable bond between the entry and exit partial structures so that they are firmly attached to each other. Also, the fluidic components attached to the resulting optical cavity structure can include, for example, connectors, tubing, pumps, sensors, and so forth; it is important that the combination of fluidic components be capable of operating to cause and control positioning of analyte within the optical cavity, such as by carrying the analyte into the optical cavity with a fluid or in some other way. The operation in box 522 can also optionally include attachment of wires or other appropriate circuitry connected, for example, to the photosensing array.

The operation in box 524 then attaches any other additional components necessary to complete the device. For example, if the device includes light sources, such as light source component 360 in FIGS. 10 and 11 or light sources 480 in FIG. 15, these components can be attached by the operation in box 524. Similarly, if a detector that includes a photosensing array and a transmission structure is not part of the exit partial structure, as in FIG. 15, the detector can be attached by the operation in box 524. The operation in box 524 can also include any other external electrical, optical, or fluidic connections necessary for operation of the device. Alternatively, such connections could later be made when the device is incorporated into a system, such as system 200 in FIGS. 7 and 8.

The operation in box 526 can be performed at any appropriate time after the other operations, as suggested by the dashed line from box 524 to box 526. In addition, the operation in box 526 performs calibration, which requires that components be appropriately connected to circuitry, such as in the ways illustrated in FIGS. 7 and 8. The necessary connections could be created as part of the operations in boxes 520, 522, and 524 or instead could be created after the operation in box 524 and before performing calibration. In any case, calibration in box 526 can include obtaining items of data or data structures to be used in obtaining analyte information as described herein, and the data or data structures can be stored in memory 246 as part of calibration data 276 (FIG. 8), or, in appropriate cases, can be embedded in analyte information routine 274 or stored in another appropriate form.

In general, the operations in any of boxes 520, 522, 524, and 526 can include additional activities. For example, at any appropriate point in production of the device, wires or other appropriate circuitry can be attached to provide signals to or from a microprocessor or input/output (I/O) device to pumps and other fluidic components or to provide signals from a photosensing array to a microprocessor or I/O device. Similarly, connections can be made at any appropriate time to provide power.

The technique of FIG. 16 could be modified in many ways within the scope of the invention. For example, the operations in boxes 520, 522, and 524 could be combined in any appropriate way to facilitate attachment of components in a desired sequence. Also, an additional operation could be performed to align or attach interconnects between ICs, gates, and other circuitry, such as connectors to a microprocessor or computer, or this operation could be partially performed in each of boxes 520, 522, 524, and 526. Furthermore, the technique of FIG. 16 is extremely general, and could be employed to produce a wide variety of different devices that encode information about optical characteristics of analyte within an optical cavity and obtain sensing results indicating the optical characteristics. The examples illustrated in FIGS. 10, 11, 14, and 15 above show how objects can be carried through a channel within an optical cavity while such operations are performed, but various other arrangements are possible, some examples of which are described below.

FIG. 17 illustrates a different type of implementation in which relative movement between analyte and photosensing array occurs, but in a manner different from the implementation in FIGS. 14 and 15. Photosensing array 550 moves relative to a biochip with an array of wells each of which can contain analyte or another fluid, such as a reference fluid; each well is represented in FIG. 17 by a shaded circle, such as circle 552. Relative motion between array 550 and the biochip is indicated by arrow 554. The biochip can, for example, be sandwiched between two mirrors (not shown) so that each well is within the optical cavity formed between the mirrors, and the cavity can be illuminated in any of various ways; the illustrated technique makes it unnecessary to perform scanning illumination, since illumination and sensing can be fully parallel. In the case, for example, in which the biochip is moved in the x-direction as indicated by arrow 554 and in which a transmission structure (not shown) over array 550 is an LVF with a gradient in the x-direction but homogeneous in the y-direction, each of the wells can pass along a respective path across the array along which sensing results are obtained for each photon energy subrange of a spectrum, allowing for step-by-step spectral characterization of the contents of each well. The wells can be correlated with their respective sensing results based on the relative velocity, similarly to the techniques described above. After all sensing results are obtained, a deconvolution of the sensing results can be performed to obtain the absorption spectrum and refractive index dispersion for each well of the biochip.

The techniques illustrated in FIGS. 14, 15, and 17 are only a few of the many possible ways of implementing relative motion between analyte in an optical cavity and a photosensing component. Additional techniques are described in co-pending U.S. patent application Ser. No. 11/702,470, entitled “Moving Analytes and Photosensors” and incorporated herein by reference in its entirety.

FIG. 18 shows setup 600, a combination of components that can be used in a system as in FIGS. 7 and 8, but possibly without an optical cavity structure as defined above; instead, a combination of components could operate as a laser cavity even though they may not be connected into a structure. Laser mirrors 602 and 604 provide reflection surfaces for the laser cavity, and gain medium 606 provides laser amplification. Duct 610, shown in dashed lines, represents a path along which objects can be carried through the laser cavity, with objects 612, 614, and 616 illustratively being carried in the direction indicated by arrows 618; objects 612, 614, and 616 could, for example, be small volumes of fluid, biological cells, or any other type of particle or object as described above.

As a result of the presence of any of objects 612, 614, and 616 in the laser cavity, emitted light represented by arrows 620 includes information about optical characteristics of analyte. Possibly after a spreading operation as described in co-pending U.S. patent application Ser. No. 11/315,387, entitled “Propagating Light to be Sensed” and incorporated herein by reference in its entirety, the analyte-affected output light is transmitted through transmission structure 622, which can be an LVF, and is photosensed by photosensing array 624. Setup 600 therefore makes it possible to obtain information, for example, about refractive index of objects 612, 614, and 616, because a change in refractive index in the laser cavity causes a shift of the emitted laser wavelength, in the manner described by Liang X. J., Liu, A. Q., Zhang, X. M., Yap, P. H., Ayi, T. C., and Yoon, H. S., “Refractive Index Measurement of Single Living Cell Using a Biophotonic Chip for Cancer Diagnosis Applications,” 9^(th) International Conference on Miniaturized Systems for Chemistry and Life Sciences, Oct. 9-13, 2005, Boston, Mass., 2005, pp. 464-466.

Setup 600 can be implemented, for example, with an external cavity laser diode. A detector that includes transmission structure 622 and array 624 can be implemented in any of the ways described above to obtain an inexpensive, compact structure that can very precisely and rapidly sense the shift of emitted laser wavelength resulting from refractive index change. By simultaneously monitoring the intensity of the laser output, analyte-induced cavity loss, such as absorption at the laser wavelength, can be recorded.

FIG. 19 shows device 650, which can also be used in a system as in FIGS. 7 and 8. Light-reflective structures 652 and 654 provide reflection surfaces on either side of region 656, which can be filled with analyte as shown. As a result, when input light, represented by arrows 658, is received through structure 652, optical cavity operation can occur, resulting in transmission of light to photosensing component 660. The index of refraction of analyte in region 656 and the positioning of structures 652 and 654 determine positions of light transmission, and illumination can be provided so that only certain wavelengths are transmitted, one of which is represented by arrow 662.

FIG. 20 shows an example of the pattern of light on the upper surface of photosensing component 660 if the optical cavity were illuminated in only one narrow wavelength band. As shown, light spot 664 on photosensing component 660 indicates that the incident narrow band light is transmitted at a certain position Xtrans. If analyte refractive index changes, the location of the transmitted light spot 364 would move, either toward Xmin or Xmax. If analyte absorption changes, causing a change in intensity and FWHM of output light's intensity function, the size and intensity of light spot 364 would change.

Inhomogeneous optical cavities that contain analyte can be implemented in many ways in addition to the way illustrated in FIGS. 19 and 20. Additional techniques are described in co-pending U.S. patent application Ser. No. 11/702,325, entitled “Containing Analyte In Optical Cavity Structures” and incorporated herein by reference in its entirety. In many applications, an optical cavity structure as in FIGS. 1 and 7 could be implemented to include one or more inhomogeneous optical cavities that contain analyte as in FIGS. 19-20. Furthermore, the optical cavity in device 650 could instead be a homogeneous optical cavity that contains analyte and that is operated to provide a laterally varying output energy distribution, by providing a range of angles at which input light is incident, as described in co-pending U.S. patent application Ser. No. 11/316,438, entitled “Photosensing Throughout Energy Range and in Subranges” and incorporated herein by reference in its entirety.

FIG. 21 shows device 680, which can also be used in a system as in FIGS. 7 and 8, such as to produce an inhomogeneous optical cavity as in FIG. 19 or to produce a tunable homogeneous or inhomogeneous cavity, including cavities through which objects can travel. Light-reflective structures 682 and 684, together with the region between them, can operate as an optical cavity when illuminated by input light, represented by arrows 686.

Structures 682 and 684 have electrodes 690 on their inward surfaces, facing each other and with elastically deformable spacers 692 and 694, such as elastomer or other deformable material, between them. As a result, signals can be provided to electrodes 690 to cause changes in distances between structures 682 and 684, changing the shape of the region between them, as suggested by angle 696. At positions where photon energy of input light is the same as a transmission mode of device 680, light is transmitted to photosensing component 698, which obtains sensing results. If analyte is present in the region between structures 682 and 684, optical cavity operation can provide analyte-affected output light. By independently addressing the electrodes on different spacers, it is also possible to keep a transmission mode's position unchanged while a neighboring mode moves further away or outside of the area of a photosensing device. This suggests how sensitivity and wavelength band can be chosen independently.

FIG. 22 illustrates an example of how device 680 can be adjusted to obtain two different transmission spectra. The intensity-energy graph in FIG. 22 includes two curves: The curve that includes peaks 710 results from a spacing of 4.8 microns between structures 682 and 684, while the curve that includes peaks 712 results from a spacing of 5 microns. Although these curves indicate operation of device 680 as a homogeneous optical cavity, similar results would occur if it were operated as an inhomogeneous cavity as illustrated in FIG. 21, though an intensity-position graph would be more appropriate in that case. In either case, the output light could include information about optical characteristics of analyte in the region between structures 682 and 684, encoded as described above in relation to FIGS. 3 and 5.

Adjustments as in FIG. 22 can be performed at different intervals with device 680 to vary the absorption sampling points as in FIG. 13. For greater resolution of an absorption spectrum, for example, the number of sampling points can be increased, and it is in principle possible to continuously vary the thickness or tilt to obtain a continuous spectrum. Furthermore, a derivative, such as of absorption, can be directly measured by recording mode intensity while continuously changing cavity thickness; sensitivity of this technique can be further increased if the thickness is periodically modulated with a small amplitude (wobble) during the continuous change of cavity thickness.

The techniques in FIGS. 21 and 22 can also be extended to obtain derivatives by calculating slope between measurements of absorption or other optical characteristics at pairs of incrementally different photon energies obtained by tuning a homogeneous optical cavity that contains analyte. Similarly, cavity shape can be adjusted by such techniques to improve sensitivity.

A device as in FIG. 21 can also be used for other purposes, such as to produce an optical cavity or transmission structure with desired characteristics. For example, a homogeneous or inhomogeneous optical cavity with desired optical thickness could be produced; similarly, a transmission structure that is an LVF with a desired gradient could be produced.

Tunable cavities that can be inhomogeneous or that can contain analyte could be implemented in many ways besides the way illustrated in relation to FIGS. 21 and 22. Additional techniques are described, for example, in co-pending U.S. patent application Ser. No. 11/702,321, entitled “Tuning Optical Cavities” and in co-pending U.S. patent application Ser. No. 11/702,320, entitled “Tuning Optical Cavities”, both of which are incorporated by reference herein in their entireties. In general, an optical cavity structure as in FIGS. 1 and 7 could be implemented to include one or more tunable cavities as in FIGS. 19-20.

FIG. 23 illustrates an application of a system as in FIGS. 7 and 8 in analyzer 750 on support structure 752, a fluidic structure. Defined in support structure 752 is serpentine channel 754 through which object 756 can travel, carried by a fluid or other appropriate substance. Object 756 can, for example, be a droplet or a small volume of fluid that includes an analyte to be analyzed.

The manner in which object 756 enters channel 754 and is carried by fluid can be the same as described in co-pending U.S. patent application Ser. No. 11/315,386, entitled “Sensing Photon Energies Emanating from Channels or Moving Objects” and incorporated herein by reference in its entirety. As explained there, object 756 can be carried through channel 754 by operation of propulsion components and can be purged or otherwise caused to exit, together with fluid that is carrying it, from one of several outlets, such as through toggling of valves. While in channel 754, object 756 can travel through a series of sensing components, each of which can obtain information about object 756.

The first two sensing components after object 756 enters channel 754 are illustratively Coulter counter 760, an electrically based particle size detector, and Mie scatter sensor 762, also a particle size detector. As mentioned above, information about size of object 756 can be used in obtaining information about its optical characteristics, and this information can be obtained from Coulter counter 760 and Mie scatter sensor 762.

The next sensing component along channel 754 is optical cavity sensor 770, shown schematically in a cross-sectional view similar to that of FIG. 11, although it would typically be implemented instead with components above and below channel 754, similarly to other sensing components described below. The schematic illustration of sensor 770 includes light-reflective components 772 and 774 and detector 776, all of which might be implemented in a variety of ways, including some of those described above. In addition, one or more light sources (not shown) could illuminate the optical cavity.

After passing through sensor 770, particle 756 can continue through subsequent sensing components, illustratively including components 782 and 784. These could, for example, include first and second fluorescence sensing components and a Raman scatter sensing component. Information obtained from any combination of the sensing components can be used to distinguish types of objects, such as different types of biological cells. Based on such a distinction, valve 790 at a bifurcation junction can be toggled between two positions, with object 756 exiting as indicating by arrow 792 if valve 790 is in one position and exiting as indicated by arrow 794 if value 790 is in another position. Examples of ways in which objects can be distinguished are described in greater detail in co-pending U.S. patent application Ser. No. 11/702,328, entitled “Distinguishing Objects” and incorporated herein by reference in its entirety.

FIG. 24 illustrates another application of a system as described above in relation to FIGS. 7 and 8. System 800 illustratively includes three components, various combinations of which could be feasibly implemented. Optical cavity component 802 receives input light from light source component 804 and, in turn, provides its output light to detector component 806. In the illustrated example, optical cavity component 802 is shown in cross-sectional view, showing how light-reflective structures 810 and 812 and wall structures 814 and 816 define two regions between light-reflective structures 810 and 812. Region 820, bounded by structures 810, 812, 814, and 816, can contain a reference fluid, while region 822, also bounded by structures 810, 812, and 816 but open at a side opposite wall structure 816, can contain fluid that enters as indicated by arrow 824.

In operation, analyte-carrying fluid, such as blood, lymph, interstitial fluid from between the cells of a human's or other organism's body, or other bodily fluid, can enter region 822 through any appropriate physical process; the analyte can be glucose, for example. As a result, optical cavity component 802 in effect operates as two parallel optical cavities: One optical cavity includes region 820 and provides output light, represented by arrow 830, with information about optical characteristics of the reference fluid (e.g. interstitial fluid with a well-known concentration); the other optical cavity includes region 822 and provides output light, represented by arrow 832, with information about a sample of fluid in which the analyte may be present. Detector 806 obtains sensing results that include both types of information and the sensing results can be provided to an external component such as a CPU or other processor, as indicated by arrow 834.

System 800 could be implemented in many different ways, and can include various optical cavity components, light sources, and detectors, including some of those described above. In addition to wristwatch-like implementations in which interstitial fluid is brought to the skin surface through small tubes or pins and then positioned in region 822, several other implementations of system 800 using implantable products are described in co-pending U.S. patent application Ser. No. 11/702,329, entitled “Implanting Optical Cavity Structures” and incorporated herein by reference in its entirety.

FIGS. 25-33 illustrate ways in which information about optical characteristics can be encoded in and obtained from output light from an optical cavity, such as in system 200 in FIGS. 7 and 8, in system 800 in FIG. 24, or in any of the other implementations described above. The techniques described in relation to FIGS. 25-33 are, however, merely illustrative, and various other techniques could be used for encoding information in an optical cavity's output light and then obtaining information from the output light, with or without intermediate operations on the output light such as transmission, reflection, focusing, spreading, filtering, or other forms of propagation or optical processing. Furthermore, the information encoded and obtained in the techniques of FIGS. 25-33 generally relates to optical characteristics of analytes, but information about other types of optical characteristics or other types of information in general could be encoded in and obtained from output light from optical cavities using techniques described herein.

FIGS. 25 and 26 illustrate one of the ways in which information about refractive index can be encoded and also suggest how information can in turn be obtained from photosensed quantities read out from a photosensing array. The transmission spectra, each with several intensity-energy peaks for respective transmission modes, were obtained by simulating a cavity similar to that described above in relation to FIG. 12, first with a refractive index n=1.30 for FIG. 25 and then with a refractive index n=1.29 for FIG. 26. Estimated intensity-energy sensing spectra of four illustrative cells of a photosensing array were then combined with the resulting transmission spectra, so that each figure shows how the intensity-energy transmission spectrum of the cavity at a respective refractive index overlaps with the intensity-energy sensing spectra of the cells.

FIG. 25 shows how sensing peak 900 overlaps very well with a transmission peak at approximately 965 nm, sensing peaks 902 and 904 do not overlap well with any of the transmission peaks, and sensing peak 906 overlaps almost perfectly with a transmission peak at 1000 nm. Then, after a change of refractive index, FIG. 26 shows that sensing peaks 900, 902, and 906 do not overlap very well with any of the transmission peaks, while sensing peak 904 now overlaps almost perfectly with a transmission peak at approximately 990 nm.

As noted above, a change in refractive index can be encoded as a shift in photon energy of a cavity's transmission or reflection modes. FIGS. 25 and 26 suggest several ways in which this encoded information can subsequently be obtained from the cavity's output light: If it is known, for example, that refractive index has one of a number of discrete values, an appropriate threshold quantity can be compared with the photosensed quantity of each cell to obtain one binary value for each cell, and these binary values would often correspond with refractive indices; in the example in FIGS. 25 and 26, a threshold could be used that would provide a binary value of 1001 for a refractive index of 1.30 and a value of 0010 for a refractive index of 1.29, with each binary value in effect indicating the extent of overlap between each of sensing peaks 900, 902, 904, and 906 with transmission peaks. Alternatively, a differential quantity could be obtained indicating a shift of wavelength in one or more of the transmission peaks, such as with the techniques described in co-pending U.S. patent application Ser. No. 11/633,302, entitled “Position-Based Response to Light” and incorporated herein by reference in its entirety; a differential quantity obtained, for example, between the cells with sensing peaks 904 and 906 could indicate a shift between refractive indices, and differential values obtained between other pairs of cells could indicate other such shifts. In general, in these and other similar techniques, an increase in the number of cells increases the amount of information obtained, allowing for redundancy that can be used for averaging and a higher confidence level.

FIGS. 27 and 28 illustrate encoding of information about absorption in an optical cavity like that described above in relation to FIG. 13. In each figure, three transmission peaks are shown at wavelengths of approximately 2.216 μm, 2.242 μm, and 2.268 μm. In FIG. 27, intensity of the peaks, normalized to overall maximum intensity Imax, is shown on a logarithmic scale, but in FIG. 28, intensity is only normalized to each peak's maximum intensity Imax (peak), which brings out the relationships between the FWHMs of the peaks.

As can be seen from FIG. 27, transmitted intensity decreases by about two orders of magnitude as absorption increases from zero to 60 per cm, with the highest peak in FIG. 27 being obtained for an absorption of zero, the lowest being obtained for an absorption of 120 per cm, and the second from the lowest being for 60 per cm. The increasing FWHM due to absorption is shown in FIG. 28 in which the order is reversed, with the upper curve being that for 120 per cm and the lowest curve being for zero absorption. As can be seen, FWHM approximately doubles if absorption doubles, such as between the second curve from the top, for 60 per cm, and the top curve, for 120 per cm.

The curves in FIGS. 27 and 28 can be related to ordinary analytes such as air and water. A density of zero corresponds, for example, with the absorption of air, so that the top peak in FIG. 27 and the lowest curve in FIG. 28 indicate the effect of no absorption when the optical cavity is filled with air. Water, on the other hand, has an absorption of approximately 30 per cm at wavelengths around 2.2 μm, so that the second peak from the top in FIG. 27 and the second lowest curve in FIG. 28 indicate absorption in an optical cavity filled with water.

The effect of an analyte in a fluidic or aerosol chamber within an air or water filled cavity can be analyzed mathematically. In general, the problem is to determine how small absorption changes will be encoded in the cavity's output light.

The transmittance T_(FP) of a Fabry-Perot optical cavity with incident light perpendicular to its entry surface is given by:

${T_{FP} = \frac{T\;\max}{1 + \left( {\frac{2F}{\pi}\sin\;\delta} \right)^{2}}},{{{where}\mspace{14mu}\delta} = \frac{2\pi\;{nw}}{\lambda}},$ the finesse F is given by:

${F = \frac{\pi\sqrt{\sqrt{R\; 1R\; 2}{\mathbb{e}}^{{- \alpha}\; w}}}{1 - {\left( \sqrt{R\; 1R\; 2} \right){\mathbb{e}}^{{- \alpha}\; w}}}},$ and the maximum transmittance Tmax is given by:

${{T\;\max} = \frac{\left( {1 - {R\; 1}} \right)\left( {1 - {R\; 2}} \right){\mathbb{e}}^{{- \alpha}\; w}}{\left( {1 - {\left( \sqrt{R\; 1R\; 2} \right){\mathbb{e}}^{{- \alpha}\; w}}} \right)^{2}}},$ with R1 and R2 being the reflectivities of the two mirrors and α being the absorption coefficient of the medium within the cavity.

FIG. 29 shows relative change in transmittance ΔT/T as a function of absorption α for several different reflectivities ranging from zero for the uppermost line to 0.999 for the lowermost and most steeply sloped line. The plotted values were obtained from the equation:

$\frac{\Delta\; T}{T} = {\frac{\left( {{T\;{\max\left( {\alpha = 0} \right)}} - {T\;{\max(\alpha)}}} \right)}{T\;{\max\left( {\alpha = 0} \right)}}.}$

The plotted values were obtained with a width w of 10 μm and a refractive index n=1.3. In effect, the uppermost line represents a conventional absorption measurement without an optical cavity (reflectivity of both mirrors is zero), while the magnitude of ΔT/T increases as reflectivity increases, causing the line with the greatest reflectivity to have the steepest slope. This is consistent with the particle theory of light under which increasing reflectivity leads to more reflections of each photon before it exits from the cavity, so that its interaction length with the analyte is extended.

An enhancement factor E indicating the increase in interaction length can be obtained from the following equation:

$E = {\frac{\frac{\Delta\; T}{T}(R)}{\frac{\Delta\; T}{T}\left( {R = 0} \right)}.}$

The enhancement factor E therefore compares the interaction length of a Fabry-Perot cavity with a conventional absorption measuring setup having zero reflectivity.

FIG. 30 is a graph showing the enhancement factor E for the same cavity as in FIG. 29 and with the same reflectivities, again plotted as a function of absorption α in an air-filled Fabry-Perot cavity. The lowest line in FIG. 30 indicates the enhancement factor E for reflectivity of zero, while the uppermost line indicates the enhancement factor E for reflectivity of 0.999. As can be seen, the enhancement factor E increases dramatically with reflectivity but remains substantially constant for a given reflectivity despite absorption changes.

FIGS. 31 and 32 are the same as FIGS. 29 and 30, but obtained for the case in which the cavity is filled with water. As a result, in FIG. 31, the negative slope of ΔT/T does not increase as rapidly with increasing reflectivity, and, in FIG. 32, the enhancement factor E similarly does not increase as rapidly with increasing reflectivity, and also decreases slightly as absorption increases across the illustrated range, at least for higher reflectivities.

FIG. 33 illustrates the relationship between photosensing array 920 and curves 922, 924, and 926, each of which is a normalized intensity function of a transmission mode in output light from a Fabry-Perot cavity. As will be understood, the result illustrated in FIG. 33 can be obtained, for example, by providing output light with an intensity-energy function having a peak, passing the output light through an LVF or other transmission structure with a laterally varying transmission function, and receiving the resulting laterally varying energy distribution on the photosensitive surface that includes the cells of array 920.

Each of curves 922, 924, and 926 is a peak with approximately the same central energy, but the intermediate intensity width (e.g. FWHM) narrows from peak 922 to peak 924 and again from peak 924 to peak 926. Therefore, the number of cells of array 920 that receive intensity above a given dynamic threshold (e.g. 50% of the maximum peak intensity) will be greater for curve 922 than for curve 924, and will similarly be greater for curve 924 than for curve 926.

As can be seen from FIG. 33, the number of cells with photosensed quantities above a defined threshold provides a measure of intermediate intensity width (e.g. FWHM) of a given mode. FIG. 33 also illustrates how cell density provides a lower limit on FWHM resolution. Because curve 926 provides above-threshold intensity for only one or perhaps two cells of array 920, its FWHM will be poorly resolved. In other words, the density of cells of array 920 is insufficient to resolve curve 926 from similar curves with slightly different FWHMs, as could otherwise be done by obtaining a Gaussian or Lorentzian fit of each curve between minima. In general, the resolution of array 920 must be sufficient that the narrowest peak obtained during normal operating conditions provides above-threshold photosensed quantities to more than one cell of array 920, as suggested in FIG. 33. In many applications, it is more convenient to use another referencing technique, such as sensing or calculating contrast-based data or another, non-width type of cavity-only absorption data, to determine absorption or absorption changes within the cavity, as described above in relation to box 306 in FIG. 9, rather than to determine FWHM or another intermediate intensity width.

As noted above in relation to FIG. 23, it is possible to integrate several analysis tools onto a single detection platform to collect information about an analyte, including sensing components for absorption, fluorescence, Raman spectroscopy, pH, and Coulter counters. It is similarly possible, and can be advantageous, to combine techniques that encode and obtain information about refractive index with techniques that encode and obtain information about optical absorption. Techniques as described above can perform both types of encoding and obtaining of information, with the result that changes in refractive index result in changed central energy of a cavity's modes, while changes in absorption spectrum cause changes in amplitude and FWHM of the cavity's modes. The relationship between refractive index and absorption follows from the definition of the complex refractive index ñ=n+iκ, where n is the refractive index and κ is the extinction coefficient. The extinction coefficient κ is related to the absorption coefficient α as follows:

$\alpha = {\frac{4{\pi\kappa}}{\lambda}.}$

Although absorption and refractive index are related to each other by the Kramers-Kronig relation, they are not really redundant. In other words, additional information can be obtained by measuring both, since, for example, a calculation of refractive index change requires information about absorption change over a very broad spectral range. Since usual measurements are made across limited spectral ranges in which refractive index changes might be strongly influenced by absorption changes in another spectral range, it is advantageous to measure both quantities separately. In particular, it is possible to obtain information about very small refractive index changes, which could not be obtained merely by measuring absorption changes.

The techniques described above also allow measurement of dispersion of refractive index, based on measurement of refractive index at each of a cavity's modes. In other words, dispersion can be obtained by measuring the shift of each mode's central energy separately.

In summary, measuring small analyte-induced refractive index changes and dispersion of refractive index can provide additional information about the analyte beyond what is available from measurement of absorption alone. Therefore, it can be advantageous to encode and obtain information about both absorption and refractive index dispersion concurrently for a desired photon energy range, and this can be done with a single system implemented as described above.

Techniques as described above also make it possible to measure local derivatives of refractive index and absorption, such as in an extinction-energy curve in which extinction κ is measured as a function of wavelength across a desired range of photon energies. The derivative of the absorption spectrum is an independent and powerful item of information that can be used to distinguish analytes; it can be used, for example, to distinguish glucose from other interstitial fluid molecules such as alanine, ascorbate, BSA, lactate, triacetin, and urea. A number of such molecules strongly influence the absorption spectrum within a wavelength band of interest for glucose, such as 2.5-2.40 μm. The derivative of the absorption spectrum of glucose, however, provides an even more characteristic differentiator from the other molecules than the absorption spectrum itself.

Glucose is an example, however, in which measurement can become more complicated. A change of glucose concentration can also change absorption at a respective narrow photon energy subrange; also, a glucose-induced absorption change that occurs throughout a broader photon energy range can correlate with a small refractive index change that slightly shifts central energy of a Fabry-Perot cavity's mode under the Kramers-Kronig relation. The transmitted intensity of the shifted mode is therefore affected both by (1) increasing or decreasing absorption and also by (2) shift to a photon energy with higher or lower intensity. Either of effects (1) and (2) can dominate, depending on the spectral position of the mode within the absorption spectrum of glucose: Effect (1) dominates at a maximum, minimum, or plateau of the absorption spectrum where dα/dλ is zero; effect (2) dominates in regions of large change within the absorption spectrum, where abs (dα/dλ)>>0, because the mode's intensity function is changing mainly due to refractive index-induced spectral shift to a region of higher or lower absorption. A detected intensity change can therefore be an indication of absorption where effect (1) dominates or an indication of derivative of absorption where effect (2) dominates.

Some implementations as described above in relation to FIG. 1-33 illustrate examples of a device that includes a photosensing component and an information obtaining component. The photosensing component can photosense output light from an optical cavity that provides light in modes, with a mode's output light including a respective intensity function. At least one mode's intensity function includes information about an optical characteristic of an analyte or of a region in the optical cavity. In response to the output light, the photosensing component provides electric signals that depend on the optical characteristic, and the information obtaining component uses the electrical signals to obtain information about the analyte or the region.

In specific implementations, the intensity functions have intensity peaks. The intensity function can include information, for example, about an optical characteristic of an analyte in the cavity, and the information obtaining component can obtain information about the optical characteristic.

Some of the implementations described above in relation to FIGS. 1-33 illustrate examples of a system that includes a photosensing component and processing circuitry. The photosensing component can photosense output light from an optical cavity as described above, providing electrical signals that depend on the optical characteristic. The processing circuitry is connected to receive the electrical signals and uses them to obtain information about the analyte or region.

In specific implementations, the processing circuitry controls an optical cavity component that includes the optical cavity.

Some of the implementations described above in relation to FIGS. 1-33 illustrate examples of a method of using optical cavities in which output light is photosensed as described above. The act of photosensing the output light includes providing electrical signals that depend on the optical characteristic and using the electrical signals to obtain information about the analyte or region.

In specific implementations, intensity of the output light is photosensed in each of a number of photon energy subranges and an electrical signal is provided indicating the photosensed intensity in each of the subranges. Information can be obtained about a refraction characteristic, an absorption characteristic, or both. For example, information can be obtained about refractive index in one set of photon energies and about optical absorption in another, different set. Furthermore, information can be obtained about an absorption spectrum and index of refraction dispersion. Where the intensity function of a mode includes an intensity peak, information can be obtained about central energy, contrast, intermediate intensity width, or maximum intensity, and different modes can have different values in each of these respects. Also, the electrical signals can be used to obtain cavity-only absorption data, including, for example, a contrast value or an intermediate intensity width value.

Some of the implementations described above in relation to FIGS. 1-33 also illustrate examples of other systems that include a photosensing component and an information obtaining component. The photosensing component photosenses light from an optical cavity that provides light with a respective intensity function for each of a set of modes, and the cavity includes a first region with a changeable optical characteristic and a second region with a reference optical characteristic. The intensity function of a mode has a feature that depends on the changeable and reference optical characteristics. The photosensing component obtains photosensed quantities indicating the feature that depends on the characteristics, and provides electrical signals indicating the photosensed quantities. The information obtaining component uses the electrical signals to obtain adjusted optical characteristic values that indicate values of the changeable optical characteristic, adjusted based on the reference optical characteristic. In specific implementations, the changeable and reference optical characteristics are absorption characteristics, such as contrast or intermediate intensity width. The information obtaining component can include processing circuitry that adjusts values of the changeable optical characteristic based on values of the reference optical characteristic.

Some of the implementations described above in relation to FIGS. 1-33 also illustrate examples of a method in which output light is photosensed as in such systems, and the resulting electrical signals are used to obtain adjusted optical characteristic values as described above.

In specific implementations, the optical characteristic values can be cavity-only absorption data, such as contrast values that the method obtains from a ratio between maximum and minimum transmittances of the cavity. The first region could contain analytes, and the method could also position an analyte in the first region and illuminate the optical cavity to provide output light, with the analyte changing the changeable optical characteristic.

Some of the implementations described above in relation to FIGS. 1-33 also illustrate examples of other systems that include a photosensing component and an information obtaining component. The photosensing component photosenses light from a sample optical cavity that provides output light in a set of modes, and a sample is present in the cavity. The photosensing component provides electrical signals that depend on whether an analyte is present in the sample: if it is, an optical characteristic of the analyte affects the intensity function of at least one mode, and the electrical signals indicate a feature of the intensity function. The information obtaining component uses the electrical signals to obtain information about presence of the analyte in the sample.

In specific implementations, a system can include an optical cavity component that includes the sample optical cavity and also a reference optical cavity that contains a reference medium. The information obtaining component can obtain an adjusted value for the analyte's presence that depends on the optical characteristic of the reference medium. The sample can, for example, include bodily fluid and the reference medium can include fluid with a known concentration of the analyte.

Some of the implementations described above in relation to FIGS. 1-33 also illustrate examples of methods in which output light is photosensed as in such systems and the electrical signals are used to obtain information about presence of the analyte in the sample.

In specific implementations, the analyte can, for example, be glucose. The sample can, for example, be bodily fluid such as interstitial fluid. The electrical signals can be used to obtain a set of derivatives of the optical characteristic as a function of photon energy, with each derivative obtained for respective subrange of photon energies different than the other derivatives. The optical characteristic can be an absorption characteristic.

The implementations in FIGS. 1-33 illustrate various applications of techniques as described above, including photosensing output light from modes of optical cavities that contain analyte or a region and obtaining information about the analyte or region, such as about its refractive index and absorption coefficient. The techniques could be readily extended to obtain information about polarization and fluorescence.

Techniques that obtain information about analytes, as exemplified by the implementations in FIGS. 1-33, can be applied in many biochip and lab-on-chip devices and in micro total analysis systems, in which a compact unit able to measure optical characteristics of analytes with high accuracy would be highly desirable. Information about refractive index and absorption, for example, could be valuable in controlling a fabrication process or a chemical reaction, for example; the controlled chemical reaction could possibly occur inside the optical cavity, allowing measurement of refractive indices and absorption coefficients even of transitory analytes resulting from the reaction. Refractive index and/or absorption index could be criteria used to make process control decisions, or could be used in a multivariable analysis, including one or more other types of information such as fluorescence or impedance.

Refractive index and absorption might be especially valuable for biological and biomedical applications. For example, the techniques described above could be used to measure optical properties (refractive index, dispersion, scattering and absorption values) of single living cells in real time without extra treatment. Similarly, the techniques could be used to measure absorption coefficient and derivative to detect glucose or other analytes in bodily fluids, such as by using an implantable product. The techniques could also be implemented in a sophisticated fluidic system, as in flow cytometry and cell sorting systems, to count, sort, separate, select, or otherwise distinguish living cells of different types that are in a medium. For example, cancerous and non-cancerous cells could be counted and/or sorted.

The techniques could be applied not only to read out biochips or as part of a complex analysis system with fluidic or aerosol channels, but also in various other applications. They can be used, for example, in fluidic sample sensing, gas sensing, aerosol sensing, and so forth.

Various of the techniques described above have been successfully implemented or simulated, including the production and operation of a highly sensitive detector that includes a commercially available IC covered with a laterally graded Fabry-Perot cavity filter on a glass slide, and that can detect, for example, wavelength shift. Changes of laser and Fabry-Perot mode intensity peaks to indicate analyte optical characteristics have been simulated.

The exemplary implementations described above allow compact, inexpensive components to rapidly and accurately perform operations such as measuring optical characteristics of fluids, biological cells, glucose, and other analytes. In general, the techniques can be implemented in existing sensors and photosensors.

The exemplary implementations described above employ optical cavities with specific parameters and modes, but a wide variety of cavities could be used. Cavities with widths in the range from a few μm to hundreds of μm are feasible, and photon energies ranging from the ultraviolet up to the far infrared could be sampled.

The exemplary implementations described above generally rely on transmission structures that include highly reflective interfaces, so that much of the incident light is reflected and only a small fraction reaches the photosensor array. Therefore, the techniques described above are especially useful in applications in which light intensity is very high or a light source emits through a large area. In addition, the above techniques make it possible to increase sensitivity by choosing simpler optics and no dispersion element. By contrast, some conventional systems such as monochromators lose all light defracted into the 0^(th), 2^(nd), and higher orders. In the implementations described above, very high light yield can be achieved by combining a transmission structure with a highly sensitive photosensor array, such as one that includes avalanche photodetectors.

In addition, components could have various shapes, dimensions, or other numerical or qualitative characteristics other than those illustrated and described above. For example, in some exemplary implementations described above, cells of a photosensor array photosense in different subranges of an application's photon energy range. The subranges of cells could have any appropriate widths and relationships, and could, for example, overlap or be distinct. The width of a cell's subrange can be chosen by designing the transmission structure and the cell sensing area; for example, the width may be as small as 0.1 nm or as great as tens of nanometers.

Some of the above exemplary implementations involve specific materials, such as in photosensor arrays or position-sensitive detectors and transmission structures, but the invention could be implemented with a wide variety of materials and with layered structures with various combinations of sublayers. In particular, photosensor arrays for a desired speed, sensitivity and wavelength range could have any suitable material, such as silicon, germanium, indium-gallium-arsenide, gallium arsenide, gallium nitride, or lead sulphide, and could be produced with any appropriate kind of devices, including, for example, photodiodes, avalanche photodiodes, p-i-n diodes, photoconductors, and so forth, with any appropriate technique for sensing and reading out information whether based on CCD, CMOS, or other techniques. Various commercially available detector arrays have pixel densities as high as ten megapixels, and some high density ICs have become relatively inexpensive.

Similarly, transmission structures could be fabricated with any appropriate techniques, including thin film technology such as sputtering, e-beam or thermal evaporation with or without plasma assistance, epitaxial growth, MBE, MOCVD, and so forth. To produce Bragg mirrors, appropriate pairs of materials with low absorption coefficients and large difference in refractive indices could be chosen, bearing in mind the photon energies of interest; exemplary materials include SiO₂/TiO₂, SiO₂/Ta₂O₅, GaAs/AlAs, and GaAs/AlGaAs. Thicknesses of layer in transmission structures may vary from 30 nm up to a few hundred nanometers.

Some of the above exemplary implementations could involve particular types of transmission structures, such as Bragg mirrors and paired distributed Bragg reflectors separated by a Fabry-Perot cavity, but, more generally, any appropriate transmission structure could be used to produce a laterally varying energy distribution. Various techniques could be used to produce transmission structures with laterally varying optical thickness in addition to those described above, including, during deposition, tilting the substrate, using a shadow mask, or using a temperature gradient to obtain graded layer thickness; also, during homogeneous deposition, off-axis doping, such as by e-beam, MBE, or MOVPE, could produce lateral variation.

Some of the above exemplary implementations use specific lasers or other light sources to obtain light with desired characteristics, but various other light source techniques could be used within the scope of the invention. Various propagation components that propagate light between other components could also be employed.

The exemplary implementation in FIGS. 8 and 9 employs a CPU, which could be a microprocessor or any other appropriate component. Furthermore, as noted above, adjustment, combining, and other operations on photosensed quantities could be done either digitally or with analog signals, and could be done either on the same IC as a photosensor array, on other components, or on a combination of the two, with any appropriate combination of software or hardware.

The above exemplary implementations generally involve production and/or use of ICs and other photosensing components, optical cavities, light sources, transmission structures, processing circuitry, and control circuitry following particular operations, but different operations could be performed, the order of the operations could be modified, and additional operations could be added within the scope of the invention. For example, in implementations in which a transmission structure is on a separate substrate from a photosensor array, the transmission structure could be moved relative to the photosensor array between consecutive monitoring operations. Also, readout of adjusted or unadjusted photosensed quantities from an IC could be performed serially or in parallel, and could be performed cell-by-cell or in a streaming operation.

While the invention has been described in conjunction with specific exemplary implementations, it is evident to those skilled in the art that many alternatives, modifications, and variations will be apparent in light of the foregoing description. Accordingly, the invention is intended to embrace all other such alternatives, modifications, and variations that fall within the spirit and scope of the appended claims. 

1. A device comprising: a photosensing component that, in use, photosenses output light from an optical cavity that provides light in a set of one or more modes; for one or more of the modes in the set, the output light including a respective intensity function; the intensity function of at least one of the modes including information about an optical absorption characteristic of an analyte present in the optical cavity or of a region of the optical cavity; in response to the output light, the photosensing component providing electrical signals that depend on the optical absorption characteristic; and an information obtaining component that uses the electrical signals to obtain information about the analyte or the region.
 2. The device of claim 1, further comprising an optical cavity structure that includes the optical cavity; the optical cavity being one of a laser and a transmissive cavity.
 3. The device of claim 2 in which the optical cavity is a Fabry-Perot cavity.
 4. The device of claim 2 in which the optical cavity provides each of the intensity functions with a respective intensity peak.
 5. The device of claim 2 in which the optical cavity is a transmissive cavity; the modes being transmission modes or reflection modes.
 6. The device of claim 1 in which the intensity function of each of the at least one of the modes includes information about an optical characteristic of an analyte present in the optical cavity, the information obtaining component obtaining information about the optical characteristic of the analyte.
 7. The device of claim 1 in which the photosensing component includes at least one of a position-sensitive detector and a photosensing array.
 8. A system that includes the device of claim 1; the information obtaining component comprising: processing circuitry that receives the electrical signals from the photosensing component; the processing circuitry using the electrical signals to obtain information about the analyte or the region.
 9. The system of claim 8 in which the processing circuitry includes a central processing unit.
 10. The system of claim 8, further comprising: an optical cavity component that includes the optical cavity; the processing circuitry further controlling the optical cavity component.
 11. A method of using optical cavities; the method comprising: photosensing output light from an optical cavity that provides light in a set of one or more modes; for one or more of the modes in the set, the output light including a respective intensity function; the intensity function of at least one of the modes including information about an optical characteristic of an analyte carried by fluid through a succession of positions in the optical cavity or about a changeable optical characteristic of a region of the optical cavity; the act of photosensing output light comprising: providing electrical signals that depend on the optical characteristic of the analyte or on the changeable optical characteristic of the region and using the electrical signals to obtain information about the analyte or the region.
 12. The method of claim 11 in which the act of photosensing further comprises: photosensing intensity of the output light from the optical cavity in each of a set of two or more photon energy subranges; the act of providing electrical signals comprising: for each of the photon energy subranges, providing an electrical signal indicating photosensed intensity.
 13. The method of claim 11 in which the act of using the electrical signals to obtain information comprises: obtaining information about the optical characteristic of the analyte.
 14. The method of claim 13 in which the act of obtaining information comprises: obtaining information about at least one of a refraction characteristic and an absorption characteristic of the analyte.
 15. The method of claim 14 in which the act of obtaining information further comprises: obtaining information about both refractive index and optical absorption of the analyte.
 16. The method of claim 11 in which the act of using the electrical signals to obtain information comprises: obtaining information about one or more of refractive index, dispersion, and absorption spectrum.
 17. The method of claim 16 in which the act of obtaining information comprises: obtaining two or more refractive index values and using the refractive index values to obtain a dispersion value.
 18. The method of claim 11 in which the act of using the electrical signals comprises: obtaining cavity-only absorption data.
 19. A method of using optical cavities; the method comprising: photosensing output light from an optical cavity that provides light in a set of one or more modes; for one or more of the modes in the set, the output light including a respective intensity function; the intensity function of at least one of the modes including information about an optical characteristic of an analyte present in the optical cavity or of a region of the optical cavity; the act of photosensing output light comprising: providing electrical signals that depend on the optical characteristic; and using the electrical signals to obtain information about the analyte or the region; the intensity function of a first one of the modes including a respective intensity peak; the act of using the electrical signals comprising obtaining information about at least one of: a central energy of the first mode's intensity peak; contrast of the first mode's intensity peak; an intermediate intensity width of the first mode's intensity peak; and a maximum intensity of the first mode's intensity peak.
 20. The method of claim 19 in which the intensity function of a second one of the modes also includes a respective intensity peak; the respective intensity peaks of the first and second modes being different in at least one of central energy, contrast, maximum intensity, and intermediate intensity width.
 21. A system comprising: a photosensing component that, in use, photosenses output light from a sample optical cavity that provides output light in a set of one or more modes, each having a respective intensity function; a fluid sample being present in the optical cavity; in response to the output light, the photosensing component providing electrical signals that depend on whether an analyte is present in the fluid sample; if the analyte is present, an optical characteristic of the analyte affecting the respective intensity function of at least one of the modes in the set, the electrical signals indicating a feature of the intensity function; and an information obtaining component that uses the electrical signals to obtain information about presence of the analyte in the fluid sample.
 22. The system of claim 21, further comprising: an optical cavity component that includes the sample optical cavity; the optical cavity component further including a reference optical cavity that contains a reference medium; the photosensing component further photosensing output light from the reference optical cavity; the electrical signals indicating an optical characteristic of the reference medium; the information obtaining component obtaining an adjusted value for the analyte's presence in the fluid sample, the adjusted value depending on the optical characteristic of the reference medium.
 23. The system of claim 22 in which the fluid sample includes bodily fluid and the reference medium includes fluid with a known concentration of the analyte.
 24. A method of using optical cavities; the method comprising: photosensing output light from an optical cavity that provides output light in a set of one or more modes, each having a respective intensity function; a sample being present in the optical cavity; the act of photosensing output light comprising: providing electrical signals that depend on whether an analyte is present in the sample; if the analyte is present, an optical absorption characteristic of the analyte affecting the respective intensity function of at least one of the modes in the set, the electrical signals indicating a feature of the intensity function; and using the electrical signals to obtain information about presence of the analyte in the sample.
 25. The method of claim 24 in which the sample is bodily fluid and the analyte is glucose.
 26. The method of claim 24 in which the act of using the electrical signals comprises: obtaining a set of one or more derivatives of the absorption characteristic as a function of photon energy; each derivative being obtained for a respective subrange of photon energies and the subranges being different.
 27. A method of using optical cavities; the method comprising: photosensing output light from an optical cavity that provides light in a set of one or more modes; for one or more of the modes in the set, the output light including a respective intensity function; the intensity function of at least one of the modes including information about an optical characteristic of an analyte present in the optical cavity or of a region of the optical cavity; the act of photosensing output light comprising: providing electrical signals that depend on the optical characteristic; and using the electrical signals to obtain information about the analyte or the region; the act of using the electrical signals comprising at least one of: obtaining information about both refractive index and optical absorption; obtaining two or more refractive index values and using the refractive index values to obtain a dispersion value; and obtaining cavity-only absorption data.
 28. The method of claim 27 in which the act of obtaining information about both refractive index and optical absorption comprises: obtaining information about refractive index at a first set of one or more photon energies; and obtaining information about optical absorption at a second set of one or more photon energies; the first and second sets of photon energies being different.
 29. The method of claim 27 in which the cavity-only absorption data include at least one of a contrast value and an intermediate intensity width value. 